BACKGROUND OF THE INVENTION AND RELATED ART
STATEMENT
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The present invention relates to a getter, a flat-panel display and a
method of producing the flat-panel display, and it relates particularly to a getter
improved in gas trapping efficiency, a flat-panel display having such a getter and
having a long lifetime and a high-quality image, and a method of easily producing
such a flat-panel display.
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In the field of displays used in television sets and information
terminals, studies have been and are made on flat-panel displays as substitutes for
conventional mainstream cathode ray tubes (CRT) for complying with demands
for a decrease in thickness, a decrease in weight, an increase in a display area and
higher fineness. As one type of the flat-panel displays, there is known a flat-panel
display having two panels opposed to each other through a vacuum layer such as a
cold cathode field emission display (FED: field emission display). In the cold
cathode field emission display (to be sometimes referred to as "display"
hereinafter), when a high electric field is applied to a top portion of, for example,
a needle-shaped conductive or semi-conductive material, electrons pass through a
potential barrier in the conductive or semi-conductive material at room
temperature due to a quantum tunnel effect and are emitted from the top portion.
This phenomenon is also called "field emission" or "cold-cathode emission".
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Fig. 66 shows a conceptual exploded view of the above display.
The display has a constitution in which a first panel P1 (display panel) and a
second panel P2 are arranged so as to be opposed to each other through a vacuum
layer and the first panel P1 and the second panel P2 are bonded to each other in
their circumferential portions through a frame 24. In Fig. 66, section lines show
bonding portions. Each of the first panel P1 and the second panel P2 is
functionally largely classified into an effective field EF1 or EF2 (indicated by
section lines) which has pixels arranged and works as an actual display portion
and a non-effective field NE1 or NE2 which encompasses the effective field EF1 or
EF2 and has peripheral circuits for selecting pixels, etc., formed thereon. For
maintaining a vacuum degree of the vacuum layer, such a display has a getter 642
composed of a material capable of trapping residual gas in the vacuum layer.
Generally, the getter 642 is disposed in the non-effective field of one of the panels
P1 and P2. In the shown example, one or a plurality of through holes 640 are
formed in the non-effective field NE1 of the first panel P1, a getter box 641 is
disposed so as to close the through hole(s) 640 from an outside of the first panel
P1, and the getter 642 is held in the getter box 641. Another through hole 616 for
vacuuming is provided in some other place of the non-effective field NE1, and
connected to the through hole 616a is a chip tube 617 which is used for sealing-off
after vacuuming.
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Fig. 67 shows a schematic partial end view of a configuration
example of a display in which electron-emitting regions constituted of a plurality
of cold cathode field emission devices (to be referred to as "field emission
devices" hereinafter) are disposed in the effective field EF1 of the first panel P1
(also called "cathode panel").
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The field emission devices shown in Fig. 67 are so-called Spindt-type
field emission devices having a conical electron-emitting portion each. Such
a field emission device comprises a supporting substrate 610, a cathode electrode
61 formed on the supporting substrate 610, an insulating layer 612 formed on the
substrate 610 and the cathode electrode 611, a gate electrode 613 formed on the
insulating layer 612, an opening portion 614 formed through the gate electrode
613 and the insulating layer 612, and a conical electron-emitting portion 615
formed on the cathode electrode 611 positioned in the bottom portion of the
opening portion 614. Generally, an electrically conductive material layer which
constitutes the cathode electrode 611 and has the form of a stripe (to be referred to
as "electrically conductive material for a cathode electrode") and an electrically
conductive material layer which constitutes the gate electrode 613 and has the
form of a stripe (to be referred to as "electrically conductive material layer for a
gate electrode") are formed in directions in which the projection images of these
electrically conductive material layers cross each other at right angles. Generally,
a plurality of the field emission devices are arranged in a region corresponding to
a portion where the projection images of the above electrically conductive
material layers in the form of stripes overlap (one region corresponds to a region
of one pixel and refers to an electron-emitting region). Further, such electron-emitting
regions are generally arranged in the effective field EF1 of the first panel
P1 in the form of a two-dimensional matrix.
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The second panel P2 (also called "anode panel") comprises a
substrate 20, fluorescent layers 21 (fluorescent layers 21R, 21G, 21B) formed on
the substrate 20 in a predetermined pattern and an anode electrode 23 formed on
the entire surface on the fluorescent layers 21. A black matrix 22 is formed on the
substrate 20 between one fluorescent layer and another fluorescent layer.
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A relatively negative voltage is applied to the cathode electrode
611 from a control circuit 30, a relatively positive voltage is applied to the gate
electrode 613 from a scanning circuit 31, and a positive voltage higher than the
voltage to the gate electrode 613 is applied to the anode electrode 23 from an
accelerating power source 32. When such a display is used for displaying, a
control signal (video signal) is inputted to the cathode electrode 611 from the
control circuit 30, and a scanning signal is inputted to the gate electrode 613 from
the scanning circuit 31. Due to an electric field generated when a voltage is
applied between the cathode electrode 611 and the gate electrode 613, electrons
are emitted from the electron-emitting portion 615 and are attracted to the anode
electrode 23 to collide with the fluorescent layer 21. As a result, the fluorescent
layer 21 is excited to emit light, whereby an intended image can be obtained.
That is, the operation of the above display is in principle controlled by a voltage
applied to the gate electrode 613 and a voltage applied to the electron-emitting
portion 615 through the cathode electrode 611.
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When the fluorescent layer 21 is irradiated with electrons in the above
display having the field emission devices, water and/or carbon dioxide caught on
the surface of, or inside, the fluorescent layer 21 acquire energy and are
dissociated or released into the vacuum layer in the form it already has or in the
form of decomposition products such as carbon monoxide, oxygen, hydrogen and
the like. The above gas which is dissociated or released into the vacuum layer
will be generically referred to as "released gas" for convenience. When the
released gas is adsorbed on the surface of the electron-emitting portion 615 or
when the adsorbed released gas is re-dissociated from the surface of the electron-emitting
portion 615, the work function of the electron-emitting portion 615
changes due to adsorption or re-dissociation, and an a result, a current of emitted
electrons varies to cause noises. For example, it is known that when oxygen gas
is adsorbed on the surface of the electron-emitting portion 615 composed of
tungsten, the work function of the surface of the electron-emitting portion 615
increases by approximately 1 or 2 eV, so that the current density of emitted
electrons decreases to approximately 10 % to 1 % based on the counterpart in a
normal state. Further, the released gas may be ionized to form a positive ion in
the vacuum layer. In this case, the positive ion is accelerated toward the electron-emitting
portion 615 due to the positive voltage applied to the anode electrode 23
through the accelerating power source 32, and the positive ion sputters the
electron-emitting portion 615 to deteriorate them.
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The above positive ion or electrons can further enter the gate
electrode 613 or the insulating layer 612 located near the electron-emitting portion
615. As a result, water, carbon dioxide, etc., adsorbed on or occluded in the gate
electrode 613 or the insulating layer 612 are dissociated or released. For this
reason, the vacuum degree near the electron-emitting portion 615 is temporarily
degraded (i.e.. an increase in pressure), and local discharge may take place
between the gate electrode 613 and the electron-emitting portion 615. If the local
discharge takes place once, sputtering of the members, which constitute the field
emission device, near the electron-emitting portion 615, an increase in the
temperature of the members and further generation of released gas proceed like a
chain reaction and the discharge is amplified, and in a worst case, the electron-emitting
portion 615 is damaged and electrons can be no longer emitted. As a
result, the lifetime of the display is degraded.
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The above getter 642 is provided for avoiding the above
disadvantages caused by the released gas. The getter 642 is composed of a
chemically highly active material such as barium, magnesium, zirconium or
titanium, and traps the gas until an equilibrium state dependent upon a partial
pressure of the released gas in the atmosphere is reached. Further, gas molecules
once trapped are diffused into the getter 642 and form a solid solution with the
material thereof, so that the trapped gas is generally not re-released in any case.
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While the getter 642 has the above excellent gas trapping
performance, it cannot be said that the getter 642 exhibits its gas trapping
performance effectively on all the field emission devices in the effective field
since it is disposed in the non-effective field of the display. That is, in most of the
field emission devices other than those field emission devices located near the
getter 642, the getter 642 cannot be expected to trap the released gas immediately
when the released gas increases a pressure near the field emission devices 615, so
that it is difficult to prevent the local discharge effectively.
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Fig. 68 schematically shows a pressure distribution example in the
vacuum layer when gas molecules are released from an electron-emitting portion
615. For example, it is supposed that gas molecules are released from a gate
electrode 613 or the insulating layer 612 in an arbitrary position D near the
electron-emitting portion 615 in the vacuum layer. In this case, the pressure in the
position D where the gas molecules are released can locally increase, for example,
up to about 1 Pa, and discharge may take place. If the position D is near the getter
box 641, the getter 642 can prevent an increase in pressure and the discharge in
the vacuum layer with its gas trapping function. However, the gas molecules are
released in the position D apart from the getter box 641 as shown in Fig. 68, the
gas trapping function of the getter 642 is poor, so that there is liable to be caused a
vicious circle in which the discharge and the release of gas molecules take place
like a chain reaction.
OBJECT AND SUMMARY OF THE INVENTION
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It is therefore an object of the present invention to provide a flat-panel
display which can attain a long lifetime and a high-quality image by
efficient gettering.
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It is another object of the present invention to provide a method of
easily producing the above flat-panel display.
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It is still another object of the present invention to provide a getter
improved in gas trapping efficiency.
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The getter of the present invention for achieving the above object
comprises a support member which is formed on a substratum and which has a
convexo-concave (or rough, uneven or irregular) surface or is constituted of a
porous material member, and a gas-trapping layer formed on the support member
in conformity with the surface of the support member.
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In the getter of the present invention, the gas-trapping layer is
formed in conformity with the surface of the support member, so that the gas-trapping
layer has an increased surface area as compared with a case where the
gas-trapping layer has a flat surface, and that the probability of contact to gas in
an external environment is high. When the getter of the present invention is
applied to the flat-panel display of the present invention to be described later, the
external environment corresponds to a vacuum layer, and the gas corresponds to
the released gas from internal constituting members which face the vacuum layer.
The getter of the present invention has excellent gas trapping efficiency over
conventional getters, and can work to maintain the vacuum degree at a high level
for a long period of time. The term "trapping" includes absorption, adsorption,
occlusion and sorption. In the getter of the present invention, further, the
substratum is not at all critical so long as it can mechanically stably support the
support member.
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The flat-panel display of the present invention for achieving the
above object is a flat-panel display comprising a first panel and a second panel
which are opposed to each other through a vacuum layer and have effective fields
where pixels are arranged, wherein the effective field of at least one of the first
panel and the second panel is provided with a getter for maintaining a vacuum
degree of the vacuum layer.
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In a specific constitution of the flat-panel display of the present
invention, the first panel has cold cathode field emission devices in the effective
field, the second panel has an anode electrode and a fluorescent layer in the
effective field, and each of the cold cathode field emission devices comprises;
- (A) an insulating layer formed on a supporting substrate,
- (B) a gate electrode formed on the insulating layer,
- (C) an opening portion which penetrates through the gate electrode
and is formed in the insulating layer, and
- (D) an electron-emitting portion formed in the opening portion, and
preferably, the above getter is provided on the gate electrode and/or
on the insulating layer between one gate electrode and another gate electrode
which are adjacent to each other.-
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The flat-panel display having the above constitution will be
referred to as "flat-panel display according to the first constitution of the present
invention". The flat-panel display according to the first constitution of the present
invention is a so-called cold cathode field emission display.
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In another specific constitution of the flat-panel display of the
present invention, the first panel has cold cathode field emission devices in the
effective field, the second panel has an anode electrode and a fluorescent layer in
the effective field, and each of the cold cathode field emission devices comprises:
- (A) an insulating layer formed on a supporting substrate,
- (B) a gate electrode formed on the insulating layer,
- (C) a second insulating layer formed on the gate electrode and the
insulating layer,
- (D) a focus electrode formed on the second insulating layer,
- (E) an opening portion which penetrates through the focus
electrode, the second insulating layer and the gate electrode and is formed in the
insulating layer, and
- (F) an electron-emitting portion formed in the opening portion, and
preferably, the above getter is provided on the focus electrode
and/or on the second insulating layer between one focus electrode and another
focus electrode which are adjacent to each other.-
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The flat-panel display having the above constitution will be
referred to as "flat-panel display according to the second constitution of the
present invention". The flat-panel display according to the second constitution of
the present invention is a cold cathode field emission display having a focus
electrode.
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The focus electrode refers to an electrode which makes it possible
to improve brightness and to prevent optical crosstalk between the adjacent pixels
by converging the path of electrons emitted through the opening portion toward
the anode electrode. In the case of a so-called high voltage type flat-panel display
in which the anode electrode and the cathode electrode have a potential difference
by the order of several kilovolts and the distance between these two electrodes is
relatively large, the focus electrode is particularly effective. A relatively negative
voltage is applied to the focus electrode from a focus power source. It is not
necessarily required to provide one focus electrode per cold cathode field
emission device. For example, the focus electrode is allowed to extend in a
predetermined arrangement direction of the cold cathode field emission devices.
In this case, a common focusing effect can be exerted on a plurality of the cold
cathode field emission devices.
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In the flat-panel display according to the first or second constitution
of the present invention, the getter comprises a support member which has a
convexo-concave surface or is constituted of a porous material member, and a
gas-trapping layer formed on the support member in conformity with the surface
of the support member. Preferably, the support member is formed on the gate
electrode and/or on the insulating layer between one gate electrode and another
gate electrode which are adjacent to each other, or it is formed on the focus
electrode and/or on the second insulating layer between one focus electrode and
another focus electrode which are adjacent to each other.
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In another specific constitution of the flat-panel display of the
present invention, the first panel has cold cathode field emission devices in the
effective field, the second panel has an anode electrode and a fluorescent layer in
the effective field, and each of the cold cathode field emission devices comprises;
- (A) an insulating layer formed on a supporting substrate,
- (B) a gate electrode which is formed on the insulating layer and at
least part of which is composed of a gas-trapping material,
- (C) an opening portion which penetrates through the gate electrode
and is formed in the insulating layer, and
- (D) an electron-emitting portion formed in the opening portion, and
preferably, the gate electrode works as the above getter.-
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The flat-panel display having the above constitution will be
referred to as "flat-panel display according to the third constitution of the present
invention". The flat-panel display according to the third constitution of the
present invention is a cold cathode field emission display.
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In the flat-panel display according to the third constitution of the
present invention, the gate electrode may have a single-layered structure
composed of a gas-trapping material, or the gate electrode may have a stacked
structure constituted, at least, of a first layer composed of an electrically
conductive material or an electrically insulating material and a second layer
composed of a gas-trapping material.
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In another specific constitution of the flat-panel display of the
present invention, the first panel has cold cathode field emission devices in the
effective field, the second panel has an anode electrode and a fluorescent layer in
the effective field, and each of the cold cathode field emission devices comprises;
- (A) an insulating layer formed on a supporting substrate,
- (B) a gate electrode formed on the insulating layer,
- (C) a second insulating layer formed on the gate electrode and on
the insulating layer,
- (D) a focus electrode which is formed on the second insulating
layer and at least part of which is composed of a gas-trapping material,
- (E) an opening portion which penetrates through the focus
electrode, the second insulating layer and the gate electrode and is formed in the
insulating layer, and
- (F) an electron-emitting portion formed in the opening portion, and
preferably, the focus electrode works as the above getter.-
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The flat-panel display having the above constitution will be
referred to as "flat-panel display according to the fourth constitution of the present
invention". The flat-panel display according to the fourth constitution of the
present invention is a cold cathode field emission display having a focus
electrode.
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In the flat-panel display according to the fourth constitution of the
present invention, the focus electrode may have a single-layered structure
composed of a gas-trapping material, or the focus electrode may have a stacked
structure constituted, at least, of a first layer composed of an electrically
conductive material or an electrically insulating material and a second layer
composed of a gas-trapping material.
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In another specific constitution of the flat-panel display of the
present invention, the first panel has cold cathode field emission devices in the
effective field, the second panel has an anode electrode and a fluorescent layer in
the effective field, and each of the cold cathode field emission devices comprises;
- (A) a spacer disposed on a supporting substrate and composed of
an electrically insulating material,
- (B) a gate electrode constituted of a gas-trapping material layer
which has a plurality of opening portions formed therein and at least part of which
is composed of a gas-trapping material, and
- (C) an electron-emitting portion formed on the supporting
substrate, and
preferably, the gas-trapping material layer is fixed such that it
comes in contact with the top surface of the spacer and that the opening portion is
positioned above the electron-emitting portion.-
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The flat-panel display having the above constitution will be
referred to as "flat-panel display according to the fifth constitution of the present
invention". The flat-panel display according to the fifth constitution of the present
invention is a cold cathode field emission display.
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In the flat-panel displays according to the first to fifth constitutions
of the present invention, the first panel is sometimes called a cathode panel, and
the second panel is sometimes called an anode panel. In the flat-panel display
according to the first constitution of the present invention, the gate electrode
and/or the insulating layer between one gate electrode and another gate electrode
which are adjacent to each other correspond to the substratum, and in the flat-panel
display according to the second constitution of the present invention, the
focus electrode and/or the second insulating layer between one focus electrode
and another focus electrode which are adjacent to each other correspond to the
substratum.
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The method of producing a flat-panel display, provided by the
present invention, for achieving the above object is a method of producing the
flat-panel display of the present invention. That is, it is a method of producing a
flat-panel display comprising a first panel and a second panel which are opposed
to each other through a vacuum layer, have effective fields where pixels are
arranged, and are bonded to each other in circumferential portions thereof, the
method including the step of forming a getter in the effective field of at least one
of the first panel and the second panel.
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In a specific constitution of the method of producing a flat-panel
display, provided by the present invention, the first panel has cold cathode field
emission devices in the effective field, the second panel has an anode electrode
and a fluorescent layer in the effective field, and the first panel can be produced
by the steps of;
- (a) forming an insulating layer on a supporting substrate,
- (b) forming an electrically conductive material layer for a gate
electrode on the insulating layer,
- (c) forming a getter-forming layer on the electrically conductive
material layer,
- (d) patterning the getter-forming layer and the electrically
conductive material layer to form a gate electrode having a getter formed on the
top surface of the gate electrode,
- (e) forming an opening portion at least in the insulating layer, and
- (f) forming or exposing an electron-emitting portion in the opening
portion.
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The method of producing a flat-panel display, having the above
constitution, will be referred to as the production method according to a first
constitution of the present invention. The flat-panel display according to the first
constitution of the present invention can be produced by the production method
according to the first constitution of the present invention, and the gate electrode
and the getter are formed by simultaneous patterning so as to have the same
patterns.
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In the production method according to the first constitution of the
present invention, preferably, the step (c) of forming a getter-forming layer
comprises (1) the step of forming a supporting member which has a convexo-concave
surface or is constituted of a porous material member, on the electrically
conductive material layer for a gate electrode, and (2) the step of forming a gas-trapping
layer which is in conformity with the surface of the supporting member,
on the supporting member.
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In another specific constitution of the method of producing a flat-panel
display, provided by the present invention, the first panel has cold cathode
field emission devices in the effective field, the second panel has an anode
electrode and a fluorescent layer in the effective field, and the first panel can be
produced by the steps of:
- (a) forming an insulating layer on a supporting substrate,
- (b) forming a gate electrode on the insulating layer,
- (c) forming a second insulating layer on the insulating layer and the
gate electrode,
- (d) forming an electrically conductive material layer for a focus
electrode on the second insulating layer,
- (e) forming a getter-forming layer on the electrically conductive
material layer,
- (f) patterning the getter-forming layer and the electrically
conductive material layer to form a focus electrode having a getter formed on the
top surface of the focus electrode,
- (g) forming an opening portion at least in the second insulating
layer and in the insulating layer, and
- (h) forming or exposing an electron-emitting portion in the opening
portion.
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The method of producing a flat-panel display, having the above
constitution, will be referred to as the production method according to a second
constitution of the present invention. The flat-panel display according to the
second constitution of the present invention can be produced by the production
method according to the second constitution of the present invention, and the
focus electrode and the getter are formed by simultaneous patterning so as to have
the same patterns.
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In the production method according to the second constitution of
the present invention, preferably, the step (e) of forming a getter-forming layer
comprises (1) the step of forming a supporting member which has a convexo-concave
surface or is constituted of a porous material member, on the electrically
conductive material layer for a focus electrode, and (2) the step of forming a gas-trapping
layer which is in conformity with the surface of the supporting member,
on the supporting member.
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In another specific constitution of the method of producing a flat-panel
display, provided by the present invention, the first panel has cold cathode
field emission devices in the effective field, the second panel has an anode
electrode and a fluorescent layer in the effective field, and the first panel can be
produced by the steps of;
- (a) forming an insulating layer on a supporting substrate,
- (b) forming a gate electrode on the insulating layer,
- (c) forming a getter on the gate electrode and/or on the insulating
layer between one gate electrode and another gate electrode which are adjacent to
each other,
- (d) forming an opening portion at least in the insulating layer, and
- (e) forming or exposing an electron-emitting portion in the opening
portion.
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The method of producing a flat-panel display, having the above
constitution, will be referred to as the production method according to a third
constitution of the present invention. The flat-panel display according to the first
constitution of the present invention can be produced by the production method
according to the third constitution of the present invention, and the gate electrode
and the getter are formed in separate steps.
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In the production method according to the third constitution of the
present invention, preferably, the step (c) of forming a getter comprises (1) the
step of forming a supporting member which has a convexo-concave surface or is
constituted of a porous material member, on the gate electrode and/or on the
insulating layer between one gate electrode and another gate electrode which are
adjacent to each other, and (2) the step of forming a gas-trapping layer which is in
conformity with the surface of the supporting member, on the supporting member.
Except for a case where the getter is formed on the entire surface, the supporting
member and the gas-trapping layer may be patterned to complete the getter after
the step (2).
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In another specific constitution of the method of producing a flat-panel
display, provided by the present invention, the first panel has cold cathode
field emission devices in the effective field, the second panel has an anode
electrode and a fluorescent layer in the effective field, and the first panel can be
produced by the steps of:
- (a) forming an insulating layer on a supporting substrate,
- (b) forming a gate electrode on the insulating layer,
- (c) forming a second insulating layer on the insulating layer and the
gate electrode,
- (d) forming a focus electrode on the second insulating layer,
- (e) forming a getter on the focus electrode and/or on the second
insulating layer between one focus electrode and another focus electrode which
are adjacent to each other,
- (f) forming an opening portion at least in the second insulating
layer and in the insulating layer, and
- (g) forming or exposing an electron-emitting portion in the opening
portion.
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The method of producing a flat-panel display, having the above
constitution, will be referred to as the production method according to a fourth
constitution of the present invention. The flat-panel display according to the
second constitution of the present invention can be produced by the production
method according to the fourth constitution of the present invention, and the focus
electrode and the getter are formed in separate steps.
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In the production method according to the fourth constitution of the
present invention, preferably, the step (e) of forming a getter comprises (1) the
step of forming a supporting member which has a convexo-concave surface or is
constituted of a porous material member, on the focus electrode and/or on the
second insulating layer between one focus electrode and another focus electrode
which are adjacent to each other, and (2) the step of forming a gas-trapping layer
which is in conformity with the surface of the supporting member, on the
supporting member. Except for a case where the getter is formed on the entire
surface, the supporting member and the gas-trapping layer may be patterned to
complete the getter after the step (2).
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In another specific constitution of the method of producing a flat-panel
display, provided by the present invention, the first panel has cold cathode
field emission devices in the effective field, the second panel has an anode
electrode and a fluorescent layer in the effective field, and the first panel can be
produced by the steps of:
- (a) forming an insulating layer on a supporting substrate,
- (b) forming a gate electrode which is at least partly composed of a
gas-trapping material and works as the getter, on the insulating layer,
- (c) forming an opening portion at least in the insulating layer, and
- (d) forming or exposing an electron-emitting portion in the opening
portion.
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The method of producing a flat-panel display, having the above
constitution, will be referred to as the production method according to a fifth
constitution of the present invention. The flat-panel display according to the third
constitution of the present invention can be produced by the production method
according to the fifth constitution of the present invention.
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In the production method according to the fifth constitution of the
present invention, the gate electrode may have a single-layered structure
composed of a gas-trapping material, or the gate electrode may have a stacked
structure constituted, at least, of a first layer composed of an electrically
conductive material or an electrically insulating material and a second layer
composed of a gas-trapping material.
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In another specific constitution of the method of producing a flat-panel
display, provided by the present invention, the first panel has cold cathode
field emission devices in the effective field, the second panel has an anode
electrode and a fluorescent layer in the effective field, and the first panel can be
produced by the steps of;
- (a) forming an insulating layer on a supporting substrate,
- (b) forming a gate electrode on the insulating layer,
- (c) forming a second insulating layer on the insulating layer and the
gate electrode,
- (d) forming a focus electrode which is at least partly composed of a
gas-trapping material and works as the getter, on the second insulating layer,
- (e) forming an opening portion at least in the second insulating
layer and in the insulating layer, and
- (f) forming or exposing an electron-emitting portion in the opening
portion.
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The method of producing a flat-panel display, having the above
constitution, will be referred to as the production method according to a sixth
constitution of the present invention. The flat-panel display according to the
fourth constitution of the present invention can be produced by the production
method according to the sixth constitution of the present invention.
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In the production method according to the sixth constitution of the
present invention, the focus electrode may have a single-layered structure
composed of a gas-trapping material, or the focus electrode may have a stacked
structure constituted, at least, of a first layer composed of an electrically
conductive material or an electrically insulating material and a second layer
composed of a gas-trapping material.
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In another specific constitution of the method of producing a flat-panel
display, provided by the present invention, the first panel has cold cathode
field emission devices in the effective field, the second panel has an anode
electrode and a fluorescent layer in the effective field, and the first panel can be
produced by the steps of;
- (a) disposing a spacer composed of an electrically insulating
material on a supporting substrate and forming an electron-emitting portion on the
supporting substrate, and
- (b) fixing a gate electrode constituted of a gas-trapping material
layer which has a plurality of opening portions formed therein and is at least
partly composed of a gas-trapping material, such that the gate electrode comes in
contact with the top surface of the spacer and that the opening portion is
positioned above the electron-emitting portion.
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The method of producing a flat-panel display, having the above
constitution, will be referred to as the production method according to a seventh
constitution of the present invention. The flat-panel display according to the third
constitution of the present invention can be produced by the production method
according to the seventh constitution of the present invention.
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In the flat-panel display according to the first constitution of the
present invention and the production method according to the third constitution of
the present invention, when the getter is formed on the gate electrode, the getter
may have the same pattern as that of the gate electrode, or the getter may have a
pattern covering the gate electrode. When the getter is formed on the gate
electrode, the supporting member and the gas-trapping layer may be composed of
either one of an electrically conductive material or an electrically insulating
material. When the getter is formed on the insulating layer between the adjacent
gate electrodes, the getter may be in contact with side surfaces of the gate
electrodes, or the getter may be spaced from the side surfaces of the gate
electrodes. However, when the getter is in contact with the side surfaces of the
gate electrodes, it is required to select materials for the supporting member and
the gas-trapping layer for preventing the short-circuiting between the adjacent
gate electrodes with the getter. It is not necessarily required to provide the getters
on the insulating layer between all of the adjacent gate electrodes. When the
getter is formed on the gate electrode and on the insulating layer between one gate
electrode and another gate electrode which are adjacent to each other, the effective
area of the getter (area which contributes to trapping the released gas) can be
secured to the largest extent. That is, as far as that portion of the supporting
member which is in contact with the gate electrode is composed of an electrically
insulating material, the getter can be formed nearly on the entire surface excluding
the opening portions even if the gas-trapping layer is composed of an electrically
conductive material.
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In the flat-panel display according to the second constitution of the
present invention and the production method according to the fourth constitution
of the present invention, when the getter is formed on the focus electrode, the
getter may have the same pattern as that of the focus electrode, or the getter may
have a pattern covering the focus electrode. When the getter is formed on the
focus electrode, the supporting member and the gas-trapping layer may be
composed of either one of an electrically conductive material or an electrically
insulating material. When the getter is formed on the second insulating layer
between the adjacent focus electrodes, the getter may be in contact with side
surfaces of the focus electrodes, or the getter may be spaced from the side surfaces
of the focus electrodes. However, when the getter is in contact with the side
surfaces of the focus electrodes, it is required to select materials for the supporting
member and the gas-trapping layer for preventing the short-circuiting between the
adjacent focus electrodes with the getter. It is not necessarily required to provide
the getter on the second insulating layer between all of the adjacent gate
electrodes. When the getter is formed on the focus electrode and on the insulating
layer between one focus electrode and another focus electrode which are adjacent
to each other, the area of the getter can be secured to the largest extent. That is, as
far as that portion of the supporting member which is in contact with the focus
electrode is composed of an electrically insulating material, the getter can be
formed nearly on the entire surface excluding the opening portions even if the
gas-trapping layer is composed of an electrically conductive material.
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In the flat-panel displays according to the first and second
constitutions of the present invention and the production methods according to the
first to fourth constitutions of the present invention, the getters may be provided to
the pixels such that one getter corresponds to one pixel, or the getters may be
provided such that one getter corresponds to a predetermined number of pixels.
When the getters are provided such that one getter corresponds to one pixel, the
getter may be provided so as to cover the entire area of the effective field. When
the getters are provided such that one getter corresponds to a predetermined
number of pixels, the layout of the getters in the effective field may be regular or
at random. Further, in the flat-panel displays according to the first and second
constitutions of the present invention and the production methods according to the
first to fourth constitutions of the present invention, the getters may be provided
such that one getter corresponds to one cold cathode field emission device (to be
referred to as "field emission device" hereinafter), or the getters may be provided
such that one getter corresponds to a predetermined number of the field emission
devices. When the getters are provided such that one getter corresponds to one
field emission device, the getter may be provided so as to cover the entire area of
the effective field. When the getters are provided such that one getter corresponds
to a predetermined number of the field emission devices the layout of the getters
in the effective field may be regular or at random. In any case, preferably, the
effective area of the getters is as large as possible, and the layout thereof has
higher regularity, for preventing the released gas from causing a local increase
pressure in the vacuum layer. In the flat-panel display of the present invention
and the flat-panel displays according to the first and second constitutions of the
present invention, the gettering efficiency is remarkably improved as compared
with any conventional flat-panel display having the getter provided in one place in
the non-effective field, so that the flat-panel displays are remarkably improved in
lifetime and image quality.
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The flat-panel display according to any one of the first to fifth
constitutions of the present invention can have any type of known cold cathode
field emission devices depending upon the layout mode of the electron-emitting
portion in the opening portion. For example, there is employed a constitution in
which a cathode electrode is formed on the supporting substrate; the insulating
layer is formed on the cathode electrode and the supporting substrate; and the
electron-emitting portion is formed on the cathode electrode positioned in the
bottom portion of the opening portion. The cold cathode field emission device
having the above electron-emitting portion on the cathode electrode includes a so-called
Spindt-type field emission device having a conical electron-emitting
portion, a so-called crown-type field emission device having a crown electron-emitting
portion and a so-called flat-type field emission device having a flat
electron-emitting portion. Otherwise, there may be employed a constitution in
which an electron-emitting layer is formed on the supporting substrate; the
insulating layer is formed on the electron-emitting layer and the supporting
substrate; and the electron-emitting layer positioned in the bottom portion of the
opening portion corresponds to the electron-emitting portion (so-called plane-type
field emission device or crater-type field emission device).
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When the flat-panel display having the above Spindt-type field
emission devices, crown-type field emission devices or flat-type field emission
devices as cold cathode field emission devices is produced by the production
method according to any one of the first to sixth constitutions of the present
invention, a cathode electrode is formed on the supporting substrate and then the
insulating layer is formed on the cathode electrode and the supporting substrate in
the step (a) of the production method according to each constitution; and the
electron-emitting portion can be formed on the cathode electrode positioned in the
bottom portion of the opening portion in the step (f) of the production method
according to first constitution, in the step (h) of the production method according
to second constitution, in the step (e) of the production method according to third
constitution, in the step (g) of the production method according to fourth
constitution, in the step (d) of the production method according to fifth
constitution, or in the step (f) of the production method according to sixth
constitution. The step (f) of the production method according to first constitution,
the step (h) of the production method according to second constitution, the step (e)
of the production method according to third constitution, the step (g) of the
production method according to fourth constitution, the step (d) of the production
method according to fifth constitution and the step (f) of the production method
according to sixth constitution will be sometimes referred to as the step of
forming the electron-emitting portion. Further, when the flat-panel display having
the plane-type field emission devices as cold cathode field emission devices is
produced by the production method according to any one of the first to sixth
constitutions of the present invention, an electron-emitting layer is formed on the
supporting substrate and then the insulating layer is formed on the electron-emitting
layer and the supporting substrate in the step (a) of the production
method according to each constitution; and the electron-emitting layer positioned
in the bottom portion of the opening portion can be exposed to expose the
electron-emitting portion in the opening portion in the step of forming the
electron-emitting portion in the production method according to each constitution.
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Otherwise, in the flat-panel display according to any one of the first
to fifth constitution of the present invention, there may be employed a constitution
in which the insulating layer covers an electron-emitting layer; the opening
portion penetrates through the electron-emitting layer; and an edge portion of the
electron-emitting layer exposed on a side wall surface of the opening portion
corresponds to the electron-emitting portion. The cold cathode field emission
device having an electron-emitting portion formed by exposing the edge portion
of the electron-emitting layer on the side wall surface of the opening portion
includes a so-called edge-type field emission device.
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When the flat-panel display having the edge-type field emission
devices as cold cathode field emission devices is produced by the production
method according to any one of the first to sixth constitutions of the present
invention, the insulating layer covering an electron-emitting layer is formed in the
step (a) of the production method according to each constitution, and an edge
portion of the electron-emitting layer is exposed on a side wall surface of the
opening portion in the step of forming the electron-emitting portion in the
production method according to each constitution.
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The above "insulating layer covering the electron-emitting layer"
includes a constitution in which the upper surface and the side surfaces of the
electron-emitting layer are covered with the insulating layer and a constitution in
which the entirety (i.e., upper surface, side surfaces and bottom surface) of the
electron-emitting layer is covered with the insulating layer. In an actual
constitution in which the entire circumference of the electron-emitting layer is
covered, there can be employed a two-layered structure constituted of an upper
insulating layer and a lower insulating layer. For example, after the lower
insulating layer is formed, the electron-emitting layer is formed on the lower
insulating layer, and then, the upper insulating layer is formed on the electron-emitting
layer and the lower insulating layer. When the insulating layer covers
only the upper surface and the side surfaces of the electron-emitting layer, the
edge portion of the electron-emitting layer is exposed on a lower side of the side
wall surface of the opening portion by forming the opening portion in the
insulating layer and the electron-emitting layer in the step (e) of the production
method according to first constitution, the step (g) of the production method
according to second constitution, the step (d) of the production method according
to third constitution, the step (f) of the production method according to fourth
constitution, the step (d) of the production method according to fifth constitution
or the step (f) of the production method according to sixth constitution. The step
(e) of the production method according to first constitution, the step (g) of the
production method according to second constitution, the step (d) of the production
method according to third constitution, the step (f) of the production method
according to fourth constitution, the step (d) of the production method according
to fifth constitution and the step (f) of the production method according to sixth
constitution will be sometimes referred to as "the step of forming the opening
portion". When the insulating layer covers the entirety of the electron-emitting
layer, the edge portion of the electron-emitting layer can be exposed on the lower
side of side wall surface of the opening portion depending upon the depth of the
opening portion by forming the opening portion in the insulating layer in the step
of forming the opening portion. When a deeper opening portion is formed, the
edge portion of the electron-emitting layer can be exposed on that side wall
surface of the opening portion which is somewhere in the depth direction of the
opening portion. When the insulating layer is formed to have a two-layered
structure constituted of the upper and lower insulating layers, there may be also
employed a constitution in which a lower gate electrode is pre-formed under the
lower insulating layer and an opening portion having the lower gate electrode
exposed in the bottom portion thereof can be formed in the insulating layer.
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In the step (e) of the production method according to the first
constitution, the step (d) of the production method according to the third
constitution and the step (c) of the production method according to the fifth
constitution, it is specified that the opening portion is formed "at least" in the
insulating layer. The reason for using the above expression is as follows. In some
cases, some through holes are formed in the getters and/or the gate electrodes (and
further, the electron-emitting layer when the edge-type field emission devices are
formed) in a step prior to the above steps, and in such cases, it is sufficient to form
the opening portion only in the insulating layer inside such a through hole. In the
step (g) of the production method according to the second constitution, the step (t)
of the production method according to the fourth constitution and the step (e) of
the production method according to the sixth constitution, it is specified that the
opening portion is formed "at least" in the second insulating layer and in the
insulating layer. The reason for using the above expression is as follows. In some
cases, some through holes are formed in the getters, the focus electrodes and/or
the gate electrodes (and further, the electron-emitting layer when the edge-type
field emission devices are formed) in a step prior to the above steps, and in such
cases, it is sufficient to form the opening portion only in the second insulating
layer and in the insulating layer inside such a through hole. As a typical method
of forming the opening portion in the insulating layer and the second insulating
layer, there can be used an etching method using a mask pattern.
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In the getter of the present invention, the flat-panel display of the
present invention, the flat-panel displays according to the first and second
constitutions of the present invention, the method of producing a flat-panel
display, provided by the present invention, and the production methods according
to the first to fourth constitutions of the present invention, the supporting member
having a convexo-concave (or rough, uneven or irregular) surface may be
constituted, for example, of nearly hemispherical silicon particles. For forming
the nearly hemispherical silicon particles, for example, there can be applied a
method of growing nearly hemispherical silicon particles for increasing a surface
area of a capacitor lower electrode (storage node electrode) in the production of
DRAM (random access memory). The formation of the nearly hemispherical
silicon particles is generally carried out according to a two-stage process
including a seeding stage and a seed-growing stage. In the seeding stage,
generally, silicon seeds (nuclei) are formed by a reduced pressure CVD method
using a silicon-containing gas. The silicon seeds are formed on the electrically
conductive material layer for a gate electrode in the production method according
to the first constitution of the present invention, on the electrically conductive
material layer for a focus electrode in the production method according to the
second constitution of the present invention, on the gate electrode and/or the
insulating layer between one gate electrode and another gate electrode which are
adjacent to each other in the production method according to the third constitution
of the present invention, and on the focus electrode and/or the second insulating
layer between one focus electrode and another focus electrode which are adjacent
to each other in the production method according to the fourth constitution of the
present invention, i.e., on the substratum. In the seed-growing stage to follow,
annealing is carried out for adhering silicon atoms to the silicon seeds and
growing the seeds to the nearly hemispherical silicon particles.
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In the getter of the present invention, the flat-panel display of the
present invention, the flat-panel displays according to the first and second
constitutions of the present invention, the method of producing a flat-panel
display, provided by the present invention, and the production methods according
to the first to fourth constitutions of the present invention, the supporting member
constituted of the nearly hemispherical silicon particles may further comprise an
amorphous silicon layer formed below the nearly hemispherical silicon particles
(i.e., on a side opposite to the side where the gas-trapping layer is to be formed).
In the method of producing a flat-panel display according to the present invention,
the above supporting member can be obtained by forming an amorphous silicon
layer beforehand in portions where the above silicon seeds are to be formed, prior
to the formation of the nearly hemispherical silicon particles. The amorphous
silicon layer can be formed, for example, by a reduced pressure CVD method. In
the surface of the amorphous silicon layer, S-H bonds formed by terminating
dangling bonds (unsaturated bonds) of silicon (Si) atoms with hydrogen (H) atoms
are present, and the hydrogen atoms in the Si-H bonds are replaced with Si atoms,
which results in easy formation of the silicon seeds.
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In the getter of the present invention, the flat-panel display of the
present invention, the flat-panel displays according to the first and second
constitutions of the present invention, the method of producing a flat-panel
display, provided by the present invention, and the production methods according
to the first to fourth constitutions of the present invention, the supporting member
may be constituted of a porous material member. The supporting member
constituted of a porous material member can consist of or formed from at least
one material selected from the group consisting of silicon oxide, silicon nitride
and silicon oxide nitride (SiON). The silicon oxide includes a so-called xerogel
having a low dielectric constant and silicon oxide containing at least one element
selected from the group consisting of phosphorus (P), boron (B) and arsenic (As)
(for example, BPSG, PSG, BSG, AsSG and PbSG).
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In the method of producing a flat-panel display, provided by the
present invention, and the production methods according to the first to fourth
constitutions of the present invention, the supporting member constituted of a
porous material member can be formed by a process including the step of forming
a supporting-member-forming film having a pyrolyzable group (group which
causes a pyrolysis under heat) or containing a solvent and the step of heat-treating
the supporting-member-forming film to pyrolyze the pyrolyzable group or to
volatilize the solvent. For example, a liquid composition prepared by dispersing a
material for the supporting member in a solvent is applied onto the substratum
(the gate electrode and/or the insulating layer between one gate electrode and
another gate electrode which are adjacent to each other, or the focus electrode
and/or the second insulating layer between one focus electrode and another focus
electrode which are adjacent to each other) to form the supporting-member-forming
film, and the supporting-member-forming film is heat-treated to volatilize
the solvent contained in the supporting-member-forming film, whereby pores can
be formed. Otherwise, the supporting member is formed from a siloxane
compound having a pyrolyzable group such as methyl group. In this case, the
pyrolyzable group is decomposed by heat treatment, and as a result, pores can be
formed.
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In the method of producing a flat-panel display, provided by the
present invention, and the production methods according to the first to fourth
constitutions of the present invention, the supporting member constituted of a
porous material member can be formed by a process including the step of forming
a supporting-member-forming film containing a plurality of components having
different etching rates, the step of heat-treating the supporting-member-forming
film to allow a plurality of the components to undergo phase separation, and the
step of removing the component having a relatively higher etching rate by
etching. While it is sufficient to use two components having different etching
rates for practical purpose, three or more components may be used. When the
number of the components is 3 or more, the number of phases caused by the phase
separation is not necessarily required to be the number of the components, and it
is sufficient to generate at least two phases. Specifically, for example, a
borosilicate glass composition containing silicon oxide (SiO2) and boron oxide
(B2O3) in an amount more than the solid solubility limit thereof in silicon oxide is
used to form the supporting-member-forming film, the boron oxide is aggregated
(phase-separated) by heat treatment, and the aggregated boron oxide is etched
with hot water, whereby pores can be formed in sites where boron oxide has
formed aggregates.
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Otherwise, in the method of producing a flat-panel display,
provided by the present invention, and the production methods according to the
first to fourth constitutions of the present invention, the supporting member
constituted of a porous material member can be formed by a process including the
step of forming a supporting-member-forming film containing a plurality of
components having different etching rates and the step of removing the
component having a relatively higher etching rate by etching. While it is
sufficient to use two components having different etching rates for practical
purpose, three or more components may be used. Specifically, for example, two
silane derivatives having different organic side chains are used to form the
supporting-member-forming film, the supporting-member-forming film is
glassified by heat treatment, and the glassified supporting-member-forming film is
etched with a diluted hydrofluoric acid aqueous solution. In this case, those
portions of the supporting-member-forming film which have a relatively higher
solubility based on the organic side chain are dissolved earlier, whereby pores can
be formed.
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In the flat-panel displays according to the third to fifth constitutions
of the present invention or the production methods thereof (production methods
according to the fifth to seventh constitutions of the present invention), the gate
electrode or the focus electrode may have a single-layered structure composed of
a gas-trapping material or may have a stacked structure constituted, at least, of a
first layer composed of an electrically conductive material or an electrically
insulating material and a second layer composed of a gas-trapping material (gas-trapping
layer). In the latter case, more preferably, the gate electrode or the focus
electrode may have a stacked structure constituted, at least, of a first layer
composed of an electrically conductive material and a second layer composed of a
gas-trapping material (gas gas-trapping layer) or a stacked structure constituted, at
least, of a first layer composed of an electrically insulating layer and a second
layer composed of an electrically conductive gas-trapping material (gas-trapping
layer). In some cases, the gate electrode or the focus electrode may have a
stacked structure constituted of a first layer composed of an electrically
conductive material, a second layer composed of an electrically insulating
material and a third layer composed of a gas-trapping material (gas-trapping layer)
or a stacked structure constituted of a first layer composed of an electrically
conductive gas-trapping material (gas-trapping layer), a second layer composed of
an electrically insulating material and a third layer composed of an electrically
conductive gas-trapping material (gas-trapping layer). Further, the gate electrode
or the focus electrode may have a stacked structure of four layers or more. When
the gate electrode or the focus electrode is formed as that having a stacked
structure, not all the portions of the gate electrode or the focus electrode are
required to have a stacked structure, and the gate electrode or the focus electrode
may partly have a stacked structure. In this case, the non-stacked portion of the
gate electrode or the focus electrode is required to have electric conductivity.
When the gate electrode or the focus electrode has a stacked structure, for
example, of two layers, the first layer and the second layer may have the same
patterns, the second layer may have a pattern covering the first layer, or the first
layer may have a pattern covering the second layer. When the first layer is
composed of an electrically conductive material, the second layer may be
composed of any one of an electrically conductive material and an electrically
insulating material. When viewed from the supporting substrate, the first layer
and the second layer may be stacked in the order of the first layer and the second
layer or in the order of the second layer and the first layer. When a stacked
structure of three layers is employed, the first layer, the second layer and the third
layer may be stacked in the order of the first layer, the second layer and the third
layer or in the order of the third layer, second layer and the first layer, when
viewed from the supporting substrate. Preferably, the outermost surface is formed
of a layer composed of a gas-trapping material in view of an increase in gas-trapping
capability.
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In the present invention, the material for the gas-trapping layer or
the gas-trapping material or the gas-trapping material layer (these will be
sometimes generically referred to as "gas-trapping material") can be selected from
materials which are already known as materials for getters. Materials for getters
are classified into so-called volatilizable materials which volatilize in a vacuum
layer and form a thin film on the surface of an internal device member to exhibit a
gettering function such as barium and so-called non-volatilizable materials which
maintain a solid state in a vacuum layer and exhibit a gettering function, such as
zirconium (Zr), titanium (Ti), zirconium-aluminum alloy, zirconium-vanadium-aluminum
alloy, zirconium-vanadium-iron alloy, a titanium-zirconium-vanadium-iron
alloy, a mixture of a zirconium powder with a graphite powder, and
magnesium. The present invention uses the non-volatilizable materials. Since the
gas-trapping layer is required to be in conformity with the surface of the
supporting member and is required to be formed on the supporting member, it is
preferred to form the gas-trapping layer by a method excellent in step coverage,
and it is also preferred to form the gas-trapping layer having such a thickness that
the convexo-concave form or pores of the supporting member surface is or are not
completely occluded. The method of forming the gas-trapping layer includes a
deposition method, a sputtering method and a CVD method. @In the flat-panel
display according to the third or fourth constitution of the present invention or the
production methods thereof, the gate electrode or the focus electrode having a
single-layered structure composed of a gas-trapping material can be also formed
by a deposition method, a sputtering method or a CVD method. In the flat-panel
display according to the fifth constitution of the present invention or the
production method thereof, the gate electrode having a single-layered structure
composed of a gas-trapping material can be formed from the above material
having the form of a band or a sheet. In the flat-panel display according to the
third or fourth constitution of the present invention or the production methods
thereof, when the gate electrode or the focus electrode has a stacked structure
constituted, at least, of a first layer composed of an electrically conductive
material or an electrically insulating material and a second layer composed of a
gas-trapping material, the first layer and the second layer can be formed by a
deposition method, a sputtering method, a CVD method or a printing method
depending upon each material. When the gate electrode or the focus electrode has
at least a two-layered structure, all portions of the gate electrode or the focus
electrode may be formed to have a two-layered structure, or all portions of the
gate electrode or the focus electrode may be constituted of a first layer and some
portions thereof may be constituted of the first layer and a second layer to have a
two-layered structure. Otherwise, all portions of the gate electrode or the focus
electrode may be constituted of a second layer and some portions thereof may be
constituted of a first layer and the second layer to have a two-layered structure. In
the flat-panel display according to the fifth constitution of the present invention or
the production method thereof, when the gate electrode or the focus electrode is
constituted, at least, of a gas-trapping layer having a stacked structure of a first
layer composed of an electrically conductive material or an electrically insulating
material and a second layer composed of a gas-trapping material, the first layer
can be constituted of a metal layer having the form of a band or a sheet and the
second layer can be formed on the first layer by a deposition method, a sputtering
method, a CVD method, a printing method or an application method, although the
method of forming these layers shall not be limited thereto. When the gas-trapping
material layer is formed to have a two-layered structure, all portions of
the gas-trapping layer may have a two-layered structure, or all portions of the gas-trapping
layer may be constituted of a first layer and some portions thereof may
be constituted of the first layer and a second layer to have a two-layered structure.
Otherwise, all portions of the gas-trapping layer are constituted of a second layer
and some portions thereof may be constituted of a first layer and the second layer
to form a two-layered structure.
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Preferably, the gas-trapping material has the property of increasing
its gas trapping capability with an increase in temperature. The temperature of
such a gas-trapping material is increased when the released gas from the
fluorescent layer and the like collides with the getter and the gate electrode or the
focus electrode, and as a result, such a gas-trapping material is improved in the
gas-trapping capability unlike any other ordinary substance which releases gas
and the like. There can be therefore overcome unstable performances caused on
the flat-panel display by an increase in temperature. Otherwise, the gas-trapping
material is preferably a material activated by heat treatment so as to have the gas-trapping
capability. The heat treatment includes irradiation of the gas-trapping
material with electron beams and heat treatment in a high-temperature furnace
having a vacuum atmosphere or an atmosphere of an inert gas such as argon or
helium. Otherwise, the gas-trapping material preferably has the property of
increasing its gas-trapping capability with an increase in temperature caused by
collision of electrons. The temperature of such a gas-trapping material is
increased when electrons collide with the getter and the gate electrode or the focus
electrode, and as a result, the gas-trapping material is improved in gas-trapping
capability unlike any other usual substance which releases gas and the like. There
can be therefore overcome unstable performances caused on the flat-panel display
by an increase in temperature. Examples of the gas-trapping material having the
property of its gas-trapping capability with an increase in temperature includes a
zirconium-aluminum alloy and a titanium-zirconium-vanadium-iron alloy.
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In the Spindt-type field emission device, the electron-emitting
portion can be composed of at least one material which is selected from the group
consisting of metals such as tungsten (W), molybdenum (Mo), titanium (Ti),
niobium (Nb), tantalum (Ta), chromium (Cr), aluminum (Al) and copper (Cu);
alloys and compounds of these metals (for example, nitrides such as TiN and
silicides such as WSi2, MoSi2, TiSi2 and TaSi2); and silicon (polysilicon or
amorphous silicon) containing an impurity. The electron-emitting portions in the
Spindt-type field emission device can be formed, for example, by a deposition
method, a sputtering method or a CVD method.
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In the crown-type field emission device, the material for the
electron-emitting portion includes electrically conductive particles and a
combination of electrically conductive particles with a binder. The material of the
electrically conductive particles includes carbon-containing materials such as
graphite; refractory metals such as tungsten (W), niobium (Nb), tantalum (Ta),
titanium (Ti), molybdenum (Mo) and chromium (Cr); and transparent electrically
conductive materials such as ITO (indium tin oxide). The binder includes glass
such as water glass and general purpose resins. Examples of the general purpose
resins include thermoplastic resins such as a vinyl chloride resin, a polyolefin
resin, a polyamide resin, a cellulose ester resin and a fluorine resin, and
thermosetting resins such as an epoxy resin, an acrylic resin and a polyester resin.
For improving electron emission efficiency, preferably, the particle size of the
electrically conductive particles is sufficiently small as compared with dimensions
of the electron-emitting portion. Although not specially limited, the form of the
electrically conductive particles is spherical, polyhedral, plate-like, acicular,
columnar or amorphous. Preferably, the electrically conductive particles have
such a form that exposed portions formed by the particles form acute projections.
Electrically conductive particles having different dimensions and different forms
may be used as a mixture. The electron-emitting portion of the crown-type field
emission device can be formed, for example, by an application method combined
with a lift-off method, a deposition method or a sputtering method.
-
In the flat-type field emission device, preferably, the electron-emitting
portion is composed of a material having a smaller work function ( than a
material for the cathode electrode. The material for the electron-emitting portion
can be selected on the basis of the work function of a material for the cathode
electrode, a potential difference between the gate electrode and the cathode
electrode, a required current density of emitted electrons, and the like. Typical
examples of the material for the cathode electrode of the field emission device
include tungsten ( = 4.55 eV), niobium ( = 4.02-4.87 eV), molybdenum ( =
4.53 - 4.95 eV), aluminum ( = 4.28 eV), copper ( = 4.6 eV), tantalum ( = 4.3
eV), chromium ( = 4.5 eV) and silicon ( = 4.9 eV). The material for electron-emitting
portion preferably has a smaller work function ( than these materials, and
the value of the work function thereof is preferably approximately 3 eV or
smaller. Examples of such a material include carbon ( < 1 eV), cesium ( = 2.14
eV), LaB6 ( = 2.66 - 2.76 eV), BaO ( = 1.6 - 2.7 eV), SrO ( = 1.25 - 1.6 eV),
Y2O3 ( = 2.0 eV), CaO ( = 1.6 - 1.86 eV), BaS ( = 2.05 eV), TiN ( = 2.92 eV)
and ZrN ( = 2.92 eV). More preferably, the electron-emitting portion is
composed of a material having a work function ( equal to, or smaller than, 2 eV.
The material for the electron-emitting portion is not necessarily required to have
electric conductivity.
-
As a material for the electron-emitting portion of the flat-type field
emission device, particularly, carbon is preferred. More specifically, diamond is
preferred, and above all, amorphous diamond is preferred. When the electron-emitting
portion is composed of amorphous diamond, an emitted electron current
density necessary for a flat-panel display can be obtained at an electric field
intensity of 5 x 107 V/m or lower. Further, since amorphous diamond is an
electric resister, emitted electron currents obtained from the electron-emitting
portions can be brought into uniform currents, and the fluctuation of brightness
can be suppressed when such field emission devices are incorporated into a tlat-panel
display. Further, since the amorphous diamond exhibit remarkably high
durability against sputtering by ions of residual gas in the flat-panel display, field
emission devices having a longer lifetime can be attained.
-
Otherwise, the material for the electron-emitting portion of the flat-type
field emission device can be selected from materials which have a secondary
electron gain δ greater than the secondary electron gain δ which the electrically
conductive material for the cathode electrode has. That is, the above material can
be properly selected from metals such as silver (Ag), aluminum (Al), gold (Au),
cobalt (Co), copper (Cu), molybdenum (Mo), niobium (Nb), nickel (Ni), platinum
(Pt), tantalum (Ta), tungsten (W) and zirconium (Zr); semiconductors such as
silicon (Si) and germanium (Ge); inorganic simple substances such as carbon and
diamond; and compounds such as aluminum oxide (Al2O3), barium oxide (BaO),
beryllium oxide (BeO), calcium oxide (CaO), magnesium oxide (MgO), tin oxide
(SnO2), barium fluoride (BaF2) and calcium fluoride (CaF2). The material for the
electron-emitting portion is not necessarily required to have electric conductivity.
-
In the plane-type field emission device, the crater-type field
emission device or the edge-type field emission device, the material for the
cathode electrode or the electron-emitting layer corresponding to the electron-emitting
portion can be selected from metals such as tungsten (W), tantalum (Ta),
niobium (Nb), titanium (Ti), molybdenum (Mo), chromium (Cr), aluminum (Al),
copper (Cu), gold (Au) and silver (Ag); alloys and compounds of these metals (for
example, nitrides such as TiN and silicides such as WSi2, Mosi2, TiSi2 and Tasi2);
semiconductors such as diamond: and a thin carbon film. Although not specially
limited, the thickness of the above cathode electrode is approximately 0.05 to 0.5
µm, preferably 0.1 to 0.3 µm. The method for forming the cathode electrode
includes deposition methods such as an electron beam deposition method and a
hot filament deposition method, a sputtering method, a combination of a CVD
method or an ion plating method with an etching method, a screen-printing
method and a plating method. When a screen-printing method or a plating
method is employed, the cathode electrodes in the form of stripes can be directly
formed.
-
In the flat-type field emission device, the plane-type field emission
device, the crater-type field emission device or the edge-type field emission
device, the cathode electrode (or an electrically conductive material layer for a
cathode electrode) or the electron-emitting portion (or the electron-emitting layer)
can be formed from an electrically conductive paste prepared by dispersing
electrically conductive fine particles. Examples of the electrically conductive fine
particles include a graphite powder; a graphite powder mixed with at least one of
metal powders such as a barium oxide powder and a strontium oxide powder;
diamond particles or a diamond-like carbon powder containing at least one of
nitrogen, phosphorus, boron and triazole; a carbon-nano-tube powder; an (Sr, Ba,
Ca)CO3 powder; and a silicon carbide powder. It is particularly preferred to select
a graphite powder as electrically conductive fine particles in view of a decrease in
threshold electric field and an improvement in durability of the electron-emitting
portion. The electrically conductive fine particles may have the form of spheres
or scales, or they may have a fixed or amorphous form. The particle diameter of
the electrically conductive fine particles is not critical so long as it is equal to, or
less than. the thickness or the pattern width of the cathode electrode or the
electron-emitting portion. With a decrease in the above particle diameter, the
number of electrons emitted per unit area can be increased. When the above
particle diameter is too small, however, the cathode electrode or the electron-emitting
portion may deteriorate in electric conductivity. The above particle
diameter is therefore preferably in the range of from 0.01 to 4.0 µm. Such
electrically conductive fine particles are mixed with a glass component or other
proper binder to prepare an electrically conductive paste, a desired pattern of the
electrically conductive paste is formed by a screen-printing method and the
pattern is calcined or sintered, whereby the cathode electrode which works as an
electron-emitting portion or the electron-emitting portion can be formed.
Otherwise, the cathode electrode which works as an electron-emitting portion or
the electron-emitting portion can be formed by a combination with a spin coating
method and an etching method.
-
In the field emission device having the Spindt-type field emission
device or the crown-type field emission device, the material for the cathode
electrode (or the electrically conductive material layer for a cathode electrode) can
be selected from metals such as tungsten (W), niobium (Nb), tantalum (Ta),
molybdenum (Mo), chromium (Cr), aluminum (Al) and copper (Cu); alloys and
compounds of these metals (for example, nitrides such as TiN and silicides such
as WSi2, MoSi2, TiSi2 and TaSi2); semiconductors such as silicon (Si); and ITO
(indium-tin oxide). The method for forming the cathode electrode includes
deposition methods such as an electron beam deposition method and a hot
filament deposition method, a sputtering method, a combination of a CVD method
or an ion plating method with an etching method, a screen-printing method and a
plating method. When a screen-printing method or a plating method is employed,
the cathode electrodes in the form of stripes can be directly formed.
-
In the flat-panel displays according to the first and second
constitutions of the present invention, materials for the cathode electrode, the gate
electrode, the upper gate electrode, the lower gate electrode and the focus
electrode can be selected from metals such as tungsten (W), niobium (Nb),
tantalum (Ta), molybdenum (Mo), chromium (Cr), aluminum (Al) and copper
(Cu); alloys and compounds of these metals (for example, nitrides such as TiN
and silicides such as WSi2, MoSi2, TiSi2 and TaSi2); semiconductors such as
silicon (Si); carbon; and ITO (indium-tin oxide). The materials for the above
electrodes may be the same or different among the electrodes. The above
electrodes can be formed by a general thin-film-forming method such as a
deposition method, a sputtering method, a CVD method, an ion plating method, a
printing method or a plating method.
-
In the flat-panel display of the present invention and the method of
producing a flat-panel display, provided by the present invention, the supporting
substrate of the first panel may be any substrate so long as its surface is composed
of an electrically insulating material. Examples of the supporting substrate
include a glass substrate, a glass substrate having a surface on which an insulating
film is formed, a quartz substrate, a quartz substrate having a surface on which an
insulating film is formed, and a semiconductor substrate having a surface on
which an insulating film is formed. The substrate of the second panel can have
the same constitution as that of the supporting substrate.
-
The material for the insulating layer, the second insulating layer,
the upper insulating layer or the lower insulating layer includes SiO2, SiN, SiON,
SOG (spin on glass) and a glass paste cured product. These materials may be
used alone or in combination. The insulating layer, the second insulating layer,
the upper insulating layer or the lower insulating layer can be formed by a known
method such as a CVD method, an application method, a sputtering method or a
printing method.
-
In the flat-panel display according to the fifth constitution of the
present invention or the production method thereof (the production method
according to the seventh aspect of the present invention), the spacer may be
formed in a region between one cathode electrode in the form of a stripe and
another cathode electrode in the form of a stripe which are adjacent to each other,
or when a plurality of the cathode electrodes are taken as one group, the spacer
may be formed in a region between one group and another group which are
adjacent to each other. In some cases, the spacer may be formed in the vicinity of
a boundary of the effective field and the non-effective field. The material for the
spacer can be selected from known electrically insulating materials. For example,
a material prepared by mixing a glass having a low melting point with a metal
oxide such as alumina can be used. The spacer can be formed, for example, by a
screen-printing method, a sandblasting method, a dry film method or a
photosensitive method. The dry film method refers to a method in which a
photosensitive film is laminated on the supporting substrate, the photosensitive
film in portions where the spacers are to be formed is removed by exposure and
development, an electrically insulating material is filled in openings formed by the
removal of the photosensitive film, and calcining or sintering of the electrically
insulating material is carried out. The photosensitive film is combusted and
removed by the calcining or sintering, and the electrically insulating material
which is filled in the openings remains to form the spacers in the form of ribs.
The photosensitive method refers to a method in which a photosensitive
electrically insulating material for the spacers is formed on the supporting
substrate, the photosensitive electrically insulating material is patterned by
exposure and development, and then calcining or sintering of the photosensitive
electrically insulating material is carried out. Alternatively, the spacer can be also
formed by a known method such as a CVD method, an application method, a
sputtering method or a printing method depending upon the material used for the
above insulating layer.
-
The opening portion of the field emission device (form obtained by
cutting the opening portion with an imaginary plane in parallel with the surface of
the supporting substrate) may have any arbitrary form such as a circle, an ellipse,
a rectangular or square form, a polygon, a roundish rectangular or square form or
a roundish polygon. The opening portion can be formed, for example, by an
isotropic etching method or a combination of anisotropic and isotropic etching
methods. In the field emission device, one electron-emitting portion may exist in
one opening portion formed in the gate electrode and the insulating layer, or a
plurality of electron-emitting portions may exist in one opening portion formed in
the gate electrode and the insulating layer. Otherwise, there may be also
employed a constitution in which a plurality of opening portions are formed in the
gate electrode, one opening portion communicating with such opening portions is
formed in the insulating layer and one or more electron-emitting portions exist in
the opening portion formed in the insulating layer.
-
In the field emission device, a resistance layer may be formed
between the cathode electrode and the electron-emitting portion. Otherwise, when
the cathode electrode surface or the edge portion of the cathode electrode
corresponds to the electron-emitting portion, that is, when the field emission
device is a plane-type field emission device or an edge-type field emission device,
the cathode electrode may have a three-layered structure constituted of an
electrically conductive material layer, a resistance layer and an electron-emitting
layer corresponding to the electron-emitting portion. The resistance layer can
stabilize performances of the field emission device and can attain uniform
electron-emitting properties. The material for the resistance layer includes
carbon-containing materials such as silicon carbide (SiC); SiN; semiconductor
materials such as amorphous silicon; and refractory metal oxides such as
ruthenium oxide (RuO2), tantalum oxide and tantalum nitride. The resistor layer
can be formed by a sputtering method, a CVD method or a screen-printing
method. The resistance value of the resistance layer is approximately 1 x 105 to 1
x 107Ω, preferably several MΩ.
-
In the flat-panel displays according to the first to fifth constitutions
of the present invention, the getter of the present invention may be provided in the
effective field of the second panel.
-
When the flat-panel displays according to the first to fifth
constitutions of the present invention are applied to cold cathode field emission
displays, general constitutions of the second panel include one type constitution in
which the anode electrode is formed on the entire surface of the substrate within
the effective field and the fluorescent layer having a predetermined form is
formed on the anode electrode and other type constitution in which the fluorescent
layer having a predetermined pattern is formed on the substrate within the
effective field and the anode electrode which also works as a metal backing is
formed entirely on the fluorescent layer and the substrate. In the former type, a
so-called metal backing layer conducting to the anode electrode may be formed on
the fluorescent layer. In the latter type, a metal backing layer may be also formed
on the anode electrode. The anode electrode may have a constitution in which the
effective field is covered with an electrically conductive material having the form
of one sheet form or in which anode electrode units each of which corresponds to
one or a plurality of electron-emitting regions are provided as a set. The
fluorescent layer is formed in the form of a stripe or dots. In a color display,
fluorescent layers which are patterned in the form of stripes or dots and
correspond to three primary colors of red (R), green (G) and blue (B) are
alternately arranged. The fluorescent layers in the form of stripes or dots are
opposed to the electron-emitting regions. A black matrix may be formed between
one fluorescent layer and another fluorescent layer which are adjacent to each
other. In any one of the flat-panel displays according to the first to fifth
constitutions of the present invention, the getter of the present invention may be
formed in a portion which is in the effective region having no fluorescent layer
formed and which faces the vacuum layer (for example, on the anode electrode).
In a practical constitution of the second panel, when a black matrix for improving
a contrast is filled in a space between the adjacent fluorescent layers, the getter of
the present invention may be provided on the black matrix or the anode electrode
positioned on the black matrix. The anode electrode can be constituted, for
example, of a metal thin film of aluminum or a transparent electrically conductive
material such as ITO (indium tin oxide).
-
In the flat-panel display or the production method thereof
according to the present invention, the getter is provided near a portion where the
released gas is generated, or the gate electrode or the focus electrode works as the
getter, so that the gas-trapping function of these can effectively prevent an
increase in pressure and discharging in the vacuum layer.
BRIEF DESCRIPTION OF THE DRAWINGS
-
The present invention will be explained with reference to drawings
hereinafter.
-
Figs. 1A, 1B and 1C show schematic constitutions of the getter of
the present invention.
-
Figs. 2A, 2B and 2C are conceptual views of the flat-panel display
of the present invention.
-
Figs. 3A, 3B, 3C and 3D are schematic end views for showing
constitutions of the cold cathode field emission device as a constituent of a flat-panel
display according to the first constitution of the present invention.
-
Figs. 4A, 4B and 4C are schematic end views for showing
constitutions of the cold cathode field emission device as a constituent of a flat-panel
display according to the first constitution of the present invention.
-
Figs. 5A and 5B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a flat-panel display in
Example 2.
-
Figs. 6A and 6B, following Fig. 5B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
flat-panel display in Example 2.
-
Figs. 7A and 7B, following Fig. 6B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
flat-panel display in Example 2.
-
Figs. 8A, 8B, 8C and 8D are schematic partial end views of a
substrate, etc., for explaining one example of the method of producing a second
panel (anode panel).
-
Fig. 9 is a schematic partial cross-sectional view of a flat-panel
display (cold cathode field emission display) in Example 2.
-
Fig. 10 is a schematic conceptual perspective view showing a
disassembled state of the first panel and the second panel of the flat-panel display
of Example 2.
-
Fig. 11 is a schematic exploded perspective view of the first panel
and the second panel of the flat-panel display of Example 2.
-
Figs. 12A and 12B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a cold cathode field
emission device as a constituent for a flat-panel display of Example 6.
-
Figs. 13A and 13B, following Fig. 12B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
cold cathode field emission device as a constituent for the flat-panel display of
Example 6.
-
Figs. 14A and 14B are schematic partial end views of the
supporting substrate, etc., for explaining the method of producing a cold cathode
field emission device as a constituent for the flat-panel display of Example 7.
-
Figs. 15A, 15B and 15C are schematic partial end views for
showing the formation pattern of a getter in Example 7.
-
Figs. 16A and 16B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a flat-panel display in
Example 8.
-
Figs. 17A, 17B and 17C are schematic partial end views for
showing the formation pattern of a getter in Example 10.
-
Figs. 18A and 18B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a flat-panel display in
Example 9.
-
Figs. 19A and 19B are schematic partial end views of variants of
the electron-emitting portion constituting the flat-panel display of Example 9.
-
Figs. 20A, 20B and 20C are schematic partial end views of variants
of the electron-emitting portion constituting the flat-panel display of Example 9.
-
Figs. 21A, 21B and 21C schematically show examples of pressure
distribution of a vacuum layer in the flat-panel display of Example 9.
-
Figs. 22A and 22B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a flat-panel display of
Example 10.
-
Fig. 23 is a schematic partial cross-sectional view of a supporting
substrate, etc., for explaining the method of producing a flat-panel display of
Example 11.
-
Fig. 24 is a characteristic diagram showing a relationship between
the temperature of a zirconium-aluminum alloy and a vacuuming rate in an
internal space in a flat-panel display.
-
Fig. 25A is a schematic partial cross-sectional view of a supporting
substrate, etc., for explaining the method of producing a flat-panel display of
Example 12, and Fig. 25B is a schematic layout of the gate electrodes, etc.
-
Figs. 26A, 26B, 26C and 26D are schematic plan views of a
plurality of opening portions of a gate electrode.
-
Figs. 27A and 27B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a crown-type field
emission device in a flat-panel display of Example 13.
-
Figs. 28A, 28B and 28C, following Fig. 27B, are schematic partial
end views of the supporting substrate, etc., for explaining the method of
producing the crown-type field emission device in the flat-panel display of
Example 13.
-
Fig. 29A following Fig. 28B, is a schematic partial end view of the
supporting substrate, etc., and Fig. 29B is a partially cut-out schematic perspective
view of the supporting substrate, etc., for explaining the method of producing the
crown-type field emission device in the flat-panel display of Example 13.
-
Figs. 30A, 30B and 30C are schematic partial cross-sectional views
of a supporting substrate, etc., for explaining the method of producing a flat-type
field emission device in a flat-panel display of Example 14.
-
Figs. 31A 31B and 31C are schematic partial cross-sectional views
of a supporting substrate, etc., for explaining the method of producing a flat-type
field emission device in a flat-panel display of Example 15.
-
Figs. 32A and 32B are schematic partial cross-sectional views of
plane-type field emission devices in a flat-panel display of Example 16.
-
Fig. 33 is a schematic partial cross-sectional view of a variant of
the plane-type field emission device in the flat-panel display of Example 16.
-
Figs. 34A and 34B are a schematic partial end view and a partial
perspective view of a supporting substrate, etc., respectively, for explaining the
-
method of producing a crater-type field emission device in a flat-panel display of
Example 17.
-
Figs. 35A and 35B, following Figs. 34A and 34B, are a schematic
partial end view and a partial perspective view of the supporting substrate, etc.,
respectively, for explaining the method of producing the crater-type field emission
device in the flat-panel display of Example 17.
-
Figs. 36A and 36B, following Figs. 35A and 35B, are a schematic
partial end view and a partial perspective view of the supporting substrate, etc.,
respectively, for explaining the method of producing the crater-type field emission
device in the flat-panel display of Example 17.
-
Figs. 37A and 37B, following Figs. 36A and 36B, are schematic
partial cross-sectional views of the supporting substrate, etc., for explaining the
method of producing the crater-type field emission device in the flat-panel display
of Example 17.
-
Figs. 38A, 38B and 38C are schematic partial cross-sectional views
of a supporting substrate, etc., for explaining the method of producing a crater-type
field emission device in a flat-panel display of Example 18.
-
Figs. 39A, 39B and 39C are schematic partial cross-sectional views
of a supporting substrate, etc., for explaining the method of producing a crater-type
field emission device in a flat-panel display of Example 19.
-
Figs. 40A and 40B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a crater-type field emission
device in a flat-panel display of Example 20.
-
Figs. 41A and 41B, following Fig. 40B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
crater-type field emission device in the flat-panel display of Example 20.
-
Figs. 42A, 42B and 42C are schematic partial cross-sectional views
of a supporting substrate, etc., for an edge-type field emission device in a flat-panel
display of Example 21.
-
Figs. 43A, 43B and 43C are schematic partial end views of the
supporting substrate, etc., for explaining the method of producing the edge-type
field emission device.
-
Figs. 44A and 44B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a Spindt-type field
emission device shown in Fig. 47 in a flat-panel display of Example 22.
-
Figs. 45A and 45B, following Fig. 44B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
Spindt-type field emission device shown in Fig. 47.
-
Figs. 46A and 46B, following Fig. 45B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
Spindt-type field emission device shown in Fig. 47.
-
Fig. 47 is a schematic partial end view of a Spindt-type field
emission device.
-
Figs. 48A and 48B show the mechanism of forming a conical
electron-emitting portion.
-
Figs. 49A, 49B and 49C schematically show relationships of a
selective ratio to a resist and the height and form of an electron-emitting portion.
-
Figs. 50A and 50B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a Spindt-type field
emission device in a flat-panel display of Example 23.
-
Figs. 51A and 51B, following Fig. 50B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
Spindt-type field emission device in the flat-panel display of Example 23.
-
Figs. 52A and 52B, following Fig. 51B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
Spindt-type field emission device in the flat-panel display of Example 23.
-
Figs. 53A and 53B show how the surface profile of a material
being etched changes per constant time period.
-
Figs. 54A and 54B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a Spindt-type field
emission device in a flat-panel display of Example 24.
-
Fig. 55 following Fig. 54B is a schematic partial end view of the
supporting substrate, etc., for explaining the method of producing the Spindt-type
field emission device in the flat-panel display of Example 24.
-
Fig. 56 is a schematic partial end view of a Spindt-type field
emission device in a flat-panel display of Example 25.
-
Figs. 57A and 57B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a Spindt-type field
emission device of Example 25.
-
Figs. 58A and 58B, following Fig. 57B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
Spindt-type field emission device of Example 25.
-
Figs. 59A and 59B, following Fig. 58B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
Spindt-type field emission device of Example 25.
-
Figs. 60A and 60B are schematic partial end views of a supporting
substrate, etc., for explaining the method of producing a Spindt-type field
emission device in a flat-panel display of Example 26.
-
Figs. 61A and 61B, following Fig. 60B, are schematic partial end
views of the supporting substrate, etc., for explaining the method of producing the
Spindt-type field emission device of Example 26.
-
Fig. 62 is a schematic partial end view of a supporting substrate,
etc., for explaining the method of producing a Spindt-type field emission device in
a flat-panel display of Example 27.
-
Fig. 63 shows one example of a driving circuit of a flat-panel
display when all of gate electrodes are constituted of one sheet-like electrode-constituting
layer.
-
Fig. 64 shows one example of a driving circuit of a flat-panel
display when all of cathode electrodes are constituted of one sheet-like electrode-constituting
layer.
-
Fig. 65 is a schematic partial end view of a flat-panel display in
which a focus electrode is provided above a gate electrode through a vacuum
layer.
-
Fig. 66 is a conceptual exploded view of a conventional flat-panel
display.
-
Fig. 67 shows a schematic layout of constituting elements in a
conventional first panel shown in Fig. 66.
-
Fig. 68 schematically shows an example of a pressure distribution
in a vacuum layer when gas molecules are released from an electron-emitting
portion in a conventional flat-panel display.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
Example 1
-
Example 1 is concerned with the getter and the flat-panel display of
the present invention. The constitution of the getter of the present invention will
be explained with reference to Figs. 1A, 1B and 1C. A getter 43A shown in Fig.
1A (to be referred to as "first-type getter 43A") comprises a supporting member
41 which is formed on a substratum 40 and has a convexo-concave surface, and a
gas-trapping layer 42 which is formed on the supporting member in conformity
with the surface of the supporting member. The supporting member in Example 1
is constituted of hemispherical silicon particles 41 (corresponding to nearly
hemispherical silicon particles). Fig. 1B shows a getter 43B (to be referred to as
"second-type getter 43B") of which the supporting member is constituted of an
amorphous silicon layer 44 formed on the substratum 40 and the hemispherical
silicon particles 41 formed on the amorphous silicon layer 44. When it is difficult
to grow the supporting member constituted of hemispherical silicon particles
directly on the surface of the substratum 40, the amorphous silicon layer 44 serves
to ease the formation of silicon seeds (nuclei) to promote the growth of the
hemispherical silicon particles 41. In a getter 43C shown in Fig. 1C (to be
referred to as "third-type getter 43C"), the supporting member is constituted of a
porous material member 45. In any one of the first-type, second type and third- type
getters 43A, 43B and 43C, the surface area of the gas-trapping layer 42
increases as compared with a case where the a gas-trapping layer has a flat
surface, so that the gas-trapping layer 42 can efficiently traps a released gas
present in an outer environment. The first-type, second-type or third- type getter
43A, 43B or 43C of the present invention can be applied to the flat-panel display
of the present invention and the flat-panel displays according to the first and
second constitutions of the present invention, and the can be also applied to a
cathode ray tube.
-
Figs. 2A, 2B and 2C show schematic constitution examples of the
flat-panel display of the present invention. In the flat-panel display shown in Fig.
2A, a first panel P1 and a second panel P2 are opposed to each other through a
vacuum layer VAC, effective regions EF1 and EF2 having pixels arranged are
provided, and a getter for maintaining the vacuum degree of the vacuum layer
VAC is provided in the effective region EF1 of the first panel P1. The first panel
P1 and the second panel P2 are bonded to each other through a seal member S in
their circumferential portions. In the flat-panel display shown in Fig. 2B, a getter
for maintaining the vacuum degree of the vacuum layer VAC is provided in the
effective region EF2 of the second panel P2. In the flat-panel display shown in
Fig. 2C, getters for maintaining the vacuum degree of the vacuum layer VAC are
provided in the effective region EF1 of the first panel P1 and the effective region
EF2 of the second panel P2. If the first panel P1 and the second panel P2 are the
cathode panel and the anode panel of a cold cathode field emission display,
respectively, the getter may be provided in the cathode panel, the anode panel or
both.
-
The seal member S may be an adhesive layer, or it may be a
combination of a frame composed of an insulating rigid material such as glass or
ceramic with an adhesive layer. When a combination of the frame with the
adhesive layer is employed, a long distance between the facing panels can be
secured by selecting a proper height of the frame as compared with a case using
an adhesive alone. While frit glass is generally used for the adhesive layer, a low-melting
metal material having a melting point of 120 to 400 °C may be used. The
low-melting metal material includes in (indium, melting point 157 °C); an
indium-gold-containing low-melting alloy; tin (Sn)-containing high-temperature
solders such as Sn80Ag20 (melting point 220 - 370 °C) and Sn95Cu5 (melting point
227 - 370 °C); lead (Pb)-containing high-temperature solders such as Pb97.5Ag2.5
(melting point 304 °C), Pb94.5Ag5.5 (melting point 304 - 365 °C) and
Pb97.5Ag1.5Sn1.0 (melting point 309 °C); zinc (Zn)-containing high-temperature
solders such as Zn95A15 (melting point 380 °C); tin-lead-containing standard
solders such as Sn2Pb98 (melting point 316 - 322 °C); and soldering materials such
as Au88Ga12 (melting point 381 °C). All of the above subscript values show
atomic %.
-
When the first panel P1, the second panel P2 and the frame are
bonded, these members may be bonded at the same time, or one of the panels and
the frame may bonded in advance at a first step and the other panel may be
bonded to the frame at a second step. When these three members are bonded at
the same time or the other panel is bonded to the frame at a second step in a
vacuum container, a space surrounded by the first panel P1, the second panel P2
and the frame comes to be a vacuum layer VAC concurrently with the bonding.
Otherwise, a space surrounded by the first panel P1, the second panel P2 and the
seal member S may be vacuumed to form a vacuum layer VAC after these three
members are bonded. When the vacuuming is carried out after the bonding, the
atmosphere for the bonding may be at atmospheric pressure or reduced pressure,
and it may be atmosphere (an air atmosphere) or an inert gas atmosphere
containing nitrogen gas or a gas coming under the group 0 of the periodic table
(for example, Ar gas).
-
When the vacuuming is carried out after the bonding, the
vacuuming can be carried out through a tip tube (not shown) pre-connected to the
first panel P1 and/or the second panel P2. Typically, the tip tube is made of a glass
tube and is bonded to a circumference of a through hole formed in a non-effective
field NE1 of the first panel P1 (i.e., an area other than the effective field EF1 which
works as a display portion) and/or to a circumference of a through hole formed in
a non-effective field NE2 of the first panel P2 (i.e., an area other than the effective
field EF2 which works as a display portion), with a frit glass or the above low-melting
metal material. After the space reaches a predetermined vacuum degree,
the gas-trapping layer or the gas-trapping material is activated, for example, by
heat treatment, and the tip tube is sealed by thermal fusion.
-
The flat-panel displays according to the first constitution of the
present invention will be explained with reference to Figs. 3A, 3B, 3C and 3D.
For simplification, these Figures show only cold cathode field emission devices
(to be referred to as "field emission device" hereinafter) and the getter formed in
the effective field EF1 of the first panel P1. The field emission device comprises a
cathode electrode 11 formed on a supporting substrate 10; an insulating layer 12
formed on the cathode electrode 11 and the supporting substrate 10; a gate
electrode 13 formed on the insulating layer 12; an opening portion 14 which
penetrates through the gate electrode 13 and is formed in the insulating layer 12;
and an electron-emitting portion 15, 15A, 15B or 15C provided on the cathode
electrode 11 positioned in a bottom portion of the opening portion 14. The first
panel P1 has a getter provided on the gate electrode 13. While the second-type
getter 43B is shown in Figures, the first type getter 43A or the third-type getter
43C may be used. The field emission device shown in Fig. 3A is a so-called
Spindt-type field emission device and has the conical electron-emitting portion
15. The field emission device shown in Fig. 3B is a crown-type field emission
device, and it has a crown-shaped electron-emitting portion 15A. The field
emission device shown in Fig. 3C is a flat-type field emission device, and it has a
flat electron-emitting portion 15B. The electron-emitting portion 15B is
composed of a material having higher electron emission efficiency than general
refractory metals, for attaining a sufficient emitted electron current in spite of
being flat. Further, the field emission device shown in Fig. 3D is a plane-type
field emission device, and an exposed portion of the cathode electrode 11 in the
bottom portion of the opening portion 14 corresponds to the electron-emitting
portion 15C.
-
The other flat-panel displays according to the first constitution of
the present invention will be explained with reference to Figs. 4A, 4B and 4C
hereinafter. For simplification, Figs. 4A to 4C show only field emission devices
(edge-type field emission device) and a getter formed in an effective field EF1 of a
first panel P1. In these Figures, the field emission device comprises an insulating
layer which is formed on a supporting substrate 10 and covers an electron-emitting
layer 111; a gate electrode 13 formed on the insulating layer; an opening
portion 14 which penetrates through the gate electrode 13 and the electron-emitting
layer 111 and is formed in the insulating layer; and an electron-emitting
portion constituted of that edge portion 111A of the electron-emitting layer 111
which is exposed on a side wall surface of the opening portion 14. The first panel
P1 further has a getter provided on the gate electrode 13. While Figs. 4A to 4C
show the second-type getter 43B, the first-type getter 43A or the second-type
getter 43C may be used. In the field emission device shown in Fig. 4A, the
insulating layer is a single-layered insulating layer 12, and the electron-emitting
layer 111 is formed in contact with the supporting substrate 10. In the field
emission device shown in Fig. 4B, the insulating layer comprises a lower
insulating layer 12A formed below the electron-emitting layer 111 and an upper
insulating layer 12B formed on the electron-emitting layer 111, and the opening
portion 14 is not only formed through the upper insulating layer 12B but also
formed so as to remove part of the lower insulating layer 12A. In the field
emission device shown in Fig. 4C, the insulating layer comprises a lower
insulating layer 12A formed below the electron-emitting layer 111 and an upper
insulating layer 12B formed on the electron-emitting layer 111, and a first gate
electrode 13A is further formed below the lower insulating layer 12A and is
exposed in a bottom portion of the opening portion 14. Further, a second gate
electrode 13B is formed on the upper insulating layer 12B. The first gate
electrode 13A serves to form a higher-intensity electric field near the edge portion
111A of the electron-emitting layer 111. The edge portion 111A corresponds to
an electron-emitting portion and is projected through the side wall surface of the
opening portion 14. Field emission devices of other types will be discussed later.
Example 2
-
Example 2 is concerned with the production method according to
the first constitution of the present invention and the flat-panel display according
to the first constitution of the present invention obtained by the above production
method. Figs. 5A, 5B, 6A, 6B, 7A, 7B and 8A to 8D show steps of the production
method of a flat-panel display (cold cathode field emission display) having a
Spindt-type field emission device shown in Fig. 3A as a typical example of the
flat-panel display according to the first constitution, and Fig. 9 shows a general
drawing of the flat-panel display. Fig. 10 shows a schematic exploded conceptual
perspective view of the flat-panel display. Fig. 11 shows a schematic exploded
perspective view of the flat-panel display.
-
In the production method in Example 2, the second-type getter 43B
shown in Fig. 1B is used as a specific example. The second-type getter 43B may
be replaced with the first-type getter 43A or the third-type getter 43C. For
simplification, Figs. 5A, 5B, 6A, 6B, 7A and 7B show only the field emission
device and the getter provided in the effective region of a first panel P1. In Figs.
6A, 6B, 7A and 7B, further, one opening portion and one electron-emitting
portion are shown per gate electrode.
-
The method of producing the Spindt-type field emission device is
basically a method in which the conical electron-emitting portion 15 is formed by
vertical deposition of a metal material. That is, vaporized particles enter
perpendicularly to the opening portion 14. The vaporized particles which reach
the bottom portion of the opening portion 14 are gradually decreased in amount
by utilizing a shielding effect of an overhanging deposit formed in the vicinity of
edge portion of the opening portion 14, whereby the electron-emitting portion 15
as a conical deposit is formed in a self-aligned manner. The method of producing
a flat-panel display having Spindt-type field emission devices on the basis of a
method in which a peel layer 18 is formed on the gate electrode 13 beforehand for
making it easy to remove the unnecessary overhanging deposit will be outlined
with reference to Figs. 5A, 5B, 6A, 6B, 7A and 7B showing schematic partial end
views of the supporting substrate, etc., and Figs. 8A to 8D showing schematic
partial cross-sectional views of the substrate, etc., of the second panel P2
hereinafter.
[Step-200]
-
First, an approximately 0.2 µm thick electrically conductive
material layer, composed of chromium, for a cathode electrode is formed on the
supporting substrate 10 made, for example, of a glass substrate. The electrically
conductive material layer is patterned in the form of stripes according to
lithography and an etching method, to form the cathode electrode 11. Then, the
insulating layer 12 is formed on the cathode electrode 11 and the supporting
substrate 10. In this Example, for example, an approximately 1 µm thick SiO2
layer is formed by a CVD method using TEOS (tetraethoxysilane) as a source gas.
Then, an electrically conductive material layer for forming gate electrodes
(electrically conductive material layer 13' for a gate electrode) is formed on the
insulating layer 12. In this Example, for example, an approximately 0.2 µm thick
chromium layer is formed as the electrically conductive material layer 13' by a
sputtering method.
-
Further, a getter-forming
layer 43 is formed on the electrically
conductive material layer 13' for a gate electrode. The getter-forming
layer 43
comprises, from the bottom, the
amorphous silicon layer 44, the
hemispherical
silicon particles 41 and the gas-trapping
layer 42 composed, for example, of an
aluminum-zirconium alloy (see Fig. 1B). The
amorphous silicon layer 44 and the
hemispherical silicon particles 41 constitute the supporting member. Table 1
shows an example of a condition for forming the
amorphous silicon layer 44 by a
reduced pressure CVD method. PH
3 may not be added. Table 2 shows one
example of a condition for forming the seeds by a reduced pressure CVD method
in the step of forming the
hemispherical silicon particles 41. Further, the gas-trapping
layer 42 composed, for example, of an aluminum-zirconium alloy is
formed on the supporting member by a sputtering method (see Fig. 5A).
[Condition for forming amorphous silicon layer] |
SiH4 flow rate | 15 SCCM |
PH3 flow rate | 2 SCCM |
Pressure | 1 x 10-3 Pa |
Forming temperature | 540 °C |
[Condition for forming seeds] |
SiH4 flow rate | 20 SCCM |
He flow rate | 30 SCCM |
Pressure | 1.33 x 10-3 Pa |
Seeds-Forming temperature | 560 °C |
[Step-210]
-
Then, an etching mask EM is formed on the getter-forming layer 43
by photolithography, and with using the etching mask EM, the getter-forming
layer 43 and the electrically conductive material layer 13' for a gate electrode are
patterned by reactive ion etching, whereby the gate electrode 13 having the
second-type getter 43B formed on its surface can be formed (see Fig. 5B).
[Step-220]
-
Then, the etching mask EM is removed, and a new etching mask
EM is formed on the second-type getter 43B and the insulating layer 12. With
using the etching mask EM, the second-type getter 43B, the gate electrode 13 and
the insulating layer 12 are consecutively etched, to form the opening portion 14
having the cathode electrode 11 exposed in its bottom portion. The opening
portion can be formed in the second-type getter 43B and the gate electrode 13 by
reactive ion etching, and the opening portion can be formed in the insulating layer
12 by wet etching with a buffered hydrofluoric acid aqueous solution. The
etching of the insulating layer 12 isotropically proceeds, so that the side wall
surface of the opening portion 14 is allowed to recede behind an end portion of
the gate electrode 13 as shown in Fig. 6A. The recess amount in this case can be
controlled on the basis of the length of an etching time period. Such a form of the
opening portion 14 is advantageous for increasing the electric field intensity in the
opening portion 14.
[Step-230]
-
Then, the etching mask EM is removed, and aluminum is obliquely
deposited on the entire surface, to form a peel layer 18 as shown in Fig. 6B. In
this case, a sufficiently large incidence angle of vaporized particles with regard to
a normal of the supporting substrate 10 is set, whereby the peel layer 18 can be
formed on the second-type getter 43B and the insulating layer 12 almost without
depositing aluminum in the bottom portion of the opening portion 14. The peel
layer 18 extends from the opening edge portion of the opening portion 14 like
eaves, whereby the opening portion 14 is substantially decreased in diameter.
[Step-240]
-
Then, for example, molybdenum (Mo) is vertically deposited on
the entire surface. In this case, with the growth of an electron-emitting-portion-forming
layer 19 having an overhanging form on the peel layer 18, the substantial
diameter of the opening portion 14 is gradually decreased, so that vaporized
particles which serve to deposition in the bottom portion of the opening portion 14
gradually come to be limited to particles which pass by the center of the opening
portion 14. As a result, as shown in Fig. 7A, a conical deposit is formed on the
cathode electrode 11 positioned in the bottom portion of the opening portion 14,
and the conical deposit constitutes the electron-emitting portion 15.
[Step-250]
-
Then, the peel layer 18 is removed together with the electron-emitting-portion-forming
layer 19 with a phosphoric acid aqueous solution,
whereby a Spindt-type field emission device as shown in Fig. 7B can be
completed.
[Step-260]
-
The first panel (cathode panel) P1 having such field emission
devices formed in a large number and the second panel (anode panel) P2 are
combined, whereby the flat-panel display can be obtained. Specifically, an
approximately 1 mm high frame 24 made, for example, of a ceramic or glass is
provided, the frame 24, the first panel P1 and the second panel P2 are bonded, for
example, with a frit glass, and the frit glass is dried, then followed by calcining or
sintering the frit glass at approximately 450 °C for 10 to 30 minutes. Then, the
inner space of the flat-panel display is vacuumed until it has a vacuum degree of
approximately 10-4 Pa, and then the gas-trapping layer (gas-trapping material) is
activated, for example, by heat treatment. Then, a tip tube 17 is sealed by a
proper method. Otherwise, the frame 24, the first panel P1 and the second panel
P2 may be bonded in a high-vacuum atmosphere. Otherwise, for some structure
of the flat-panel display, the first panel P1 and the second panel P2 may be bonded
to each other without the frame.
-
One example of the method of producing the second panel P, will
be explained with reference to Figs. 8A to 8D below. First, a composition of
light-emitting crystal particles is prepared. For example, a dispersing agent is
dispersed in pure water, and the dispersion is stirred with a homomixer at 3000
rpm for 1 minute. Then, light-emitting crystal particles are poured into the pure
water with the dispersing agent, and the mixture is stirred with a homomixer at
5000 rpm for 5 minutes. Then, for example, polyvinyl alcohol and ammonium
bichromate are added, and the mixture is fully stirred and filtered.
-
In the production of the second panel P2, a photosensitive film 25 is
formed (applied) on the entire surface of the substrate 20 made, for example, of a
glass. The photosensitive film 25 is exposed to light which comes from a light
source (not shown) and passes through an opening 29 formed in a mask 28, to
form an exposed region 26 (see Fig. 8A). Then, the photosensitive film 25 is
selectively removed by development, to retain a remaining portion 27 of the
photosensitive film (exposed and developed photosensitive film) on the substrate
20 (see Fig. 8B). Then, a carbon agent (carbon slurry) is applied onto the entire
surface, and the applied carbon agent is dried and calcined or sintered. Then, the
remaining portion 27 of the photosensitive film and the carbon agent thereon are
removed by a lift-off method, to form a black matrix 22 composed of the carbon
agent on the exposed substrate 20 (see Fig. 8C). Then, red, green and blue
fluorescent layers 21 are formed on the exposed substrate 20 (see Fig. 8D).
Specifically, compositions of light-emitting crystal particles are prepared from the
light-emitting crystal particles (fluorescent particles). For example, a
photosensitive composition of red light-emitting crystal particles (fluorescent
material slurry) is applied onto the entire surface, followed by exposure and
development. A photosensitive composition of green light-emitting crystal
particles (fluorescent material slurry) is applied onto the entire surface, followed
by exposure and development. Further, a photosensitive composition of blue
light-emitting crystal particles (fluorescent material slurry) is applied onto the
entire surface, followed by exposure and development. Then, an anode electrode
23 is formed on the fluorescent layers 21 and the black matrix 22 by a sputtering
method. The anode electrode 23 is constituted of an aluminum thin film having a
thickness of approximately 0.07 µm. Alternatively, each fluorescent layer 21 can
be formed by a screen-printing method or the like.
-
Fig. 9 shows a constitution example of the flat-panel display of
Example 2. While Fig. 9 shows one opening portion 14 and two electron-emitting
portions 15 per one line of the gate electrode 13, the basic constitution of the
Spindt-type field emission device is as shown in Fig. 7B. The above Spindt-type
field emission devices are formed in the effective field EF1 of the first panel P1
(also called a cathode panel). The second panel P2 (also called an anode panel)
comprises the substrate 20, the fluorescent layers 21 (fluorescent layers 21R, 21G,
21B) formed on the substrate 20 according to predetermined patterns and the
anode electrode 23 formed on the entire surfaces of the fluorescent layers 21. The
black matrix 22 is filled between one fluorescent layer 21 and another fluorescent
layer 21 which are adjacent to each other, for improving a contrast.
-
As Fig. 10 shows a conceptual exploded view of the flat-panel
display, in the flat-panel display of Example 2, the first panel P1 (display panel)
and the second panel P2 are opposed to each other through the vacuum layer VAC
and bonded to each other through the frame 24 in their circumferential portions.
Fig. 10 indicates the bonding portion with section lines. Each of the first panel P1
and the second panel P2 is functionally largely classified into the effective field
EF1 or EF2 (indicated by slanting lines) which has the pixels arranged therein and
works as an actual display portion and a non-effective field NE1 or NE2 which
surrounds the effective field EF1 or EF2 and has peripheral circuits, etc., for
selecting the pixels. Other through hole 16 for vacuuming is provided in the non-effective
field NE1, and the tip tube 17 which is to be sealed after vacuuming is
connected to the through hole 16. The vacuum layer VAC has a vacuum degree
on the order of 10-4 to 10-6 Pa.
-
As shown in Fig. 11, an electrically conductive material layer for a
cathode electrode in the form of a stripe (electrically conductive material layer for
a cathode electrode) and an electrically conductive material layer for a gate
electrode in the form of a stripe are formed in directions in which the projection
images of these layers cross each other at right angles. In Example 2, a plurality
of the field emission devices are arranged in a region where the projection images
of the above layers in the form of stripes overlap. Such a region corresponds to
one pixel and is an electron-emitting region. Further, such electron-emitting
regions are generally arranged in the effective field EF1 of the first panel P1 so as
to form a two-dimensional matrix. One pixel comprises the electron-emitting
region (having a plurality of field emission devices) where the electrically
conductive material layer for a cathode electrode and the electrically conductive
material layer for a gate electrode overlap and the fluorescent layer 21 which faces
the electron-emitting region. In the effective fields EF1 and EF2, for example,
such pixels on the order of hundreds of thousands to millions are arranged in the
form of a two-dimensional matrix.
-
A relatively negative voltage is applied to the cathode electrode 11
from a scanning circuit 30, a relatively positive voltage is applied to the gate
electrode 13 from a control circuit 31, and a positive voltage higher than the
voltage applied to the gate electrode 13 is applied to the anode electrode 23 from
an acceleration power source 32. When such a flat-panel display displays an
image, a scanning signal is inputted to the cathode electrode 11 from the scanning
circuit 30, and a video signal is inputted to the gate electrode 13 from the control
circuit 31. When the gate electrode 13 and the cathode electrode 11 come to have
a potential difference ΔV equal to, or higher than, a certain threshold voltage Vth,
the potential difference ΔV causes an electric field, and on the basis of the electric
field, electrons are emitted from the top end of the electron-emitting portion 15
owing to a quantum tunnel effect.
-
In the flat-panel display of Example 2, specifically, the electron-emitting
regions arranged in the row direction (X-direction) are consecutively
operated in the column direction (Y-direction). That is, a constant voltage VG
from the scanning circuit 31 is applied consecutively to the electrically conductive
material layers for a gate electrode in the form of stripes where the gate electrodes
13 are formed. On the other hand, a voltage of 0 ≤ [VC-MAX to VC-MIN] (<VG)
from the control circuit 30 is applied to each of the electrically conductive
material layers for a cathode electrode in the form of stripes where the cathode
electrodes 11 are formed. In a region where the electrically conductive material
layer for a gate electrode in the form of a stripe where the voltage VG is applied
and the electrically conductive material layer for a cathode electrode in the form
of a stripe where the voltage of VC-MAX to VC-MIN is applied overlap, the potential
difference ΔV comes to be the largest at (VG - VC-MIN), the amount of electrons
emitted from the electron-emitting region comes to be the largest, and the
electrons are attracted to the anode electrode 23 and collide with the fluorescent
layer 21. A positive voltage higher than the voltage applied to the gate electrode
13 is applied to the anode electrode 23 from the acceleration power source 32. As
a result, the fluorescent layer corresponding to such an electron-emitting region
come to show a highest brightness. On the other hand, in (VG - VC-MAX), the
potential difference ΔV comes to be the smallest, no electrons are emitted from
the electron-emitting region, and the fluorescent layer corresponding to such an
electron-emitting region emit no light. By applying a voltage of VC-MAX to VC-MIN
to each electrically conductive material layer for a cathode electrode, the
brightness of the fluorescent layer can be controlled.
-
In the flat-panel display having the above constitution, the second-type
getters 43B are provided in the effective field EF1 of the first panel P1, more
specifically, on the gate electrodes 13, so that a uniform gas-trapping effect can be
secured for the Spindt-type field emission devices positioned all over in the
effective field. In the above flat-panel display, local discharging and damaging of
electron-emitting portions are prevented, and a longer lifetime and high-quality
images can be achieved.
Example 3
-
Example 3 is a variant of Example 2. Example 3 differs from
Example 2 mainly in that the third-type getters 43C each having a supporting
member constituted of a porous material member 45 are formed.
-
Procedures up to the formation of the electrically conductive
material layer 13' for a gate electrode are carried out in the same manner as in
[Step-200] of Example 2, except that ITO is used as a material for a
cathode
electrode 11. Then, the getter-forming
layer 43 is formed on the electrically
conductive material layer 13' for a gate electrode. The getter-forming
layer 43
comprises, from a lower layer side, the supporting member constituted of the
porous material member 45 and the gas-trapping
layer 42 formed on the porous
material member 45 (see Fig. 1C). In Example 3, for example, a methylsiloxane
solution is applied onto the entire surface by a spin coating method at 3000 rpm,
and the obtained supporting-member-forming film is calcined or sintered around
500 °C, to form the
porous material member 45 composed of silicon-oxide-containing
xerogel. Then, the gas-trapping
layer 42 composed of titanium (Ti) is
formed on the
porous material member 45, for example, by a sputtering method or
a CVD method. Table 3 shows one example of a condition for forming the gas-trapping
layer 42 composed of titanium (Ti) by a CVD method. Procedures to
come thereafter can be carried out in the same manner as in Example 2 except that
tungsten is used to form the electron-emitting
portions 15. In Example 3, the tlat-panel
display shown in Figs. 9 to 11 can be constituted as well.
[Condition for forming gas-trapping layer composed of titanium (Ti)] |
CVD Apparatus | Magnetic-field-possessing microwave plasma CVD apparatus |
TiCl |
4 | 15 SCCM |
H2 flow rate | 50 SCCM |
Ar flow rate | 43 SCCM |
Pressure | 0.3 Pa |
Microwave power | 2.0 kW (2.45 GHz) |
Forming temperature | 420 °C |
Example 4
-
Example 4 is a variant of Example 3. Example 4 differs from
Example 3 mainly in that the porous material member 45 is formed by utilizing
phase separation. In the step of forming the porous material member 45, first, for
example, TEOS and trimethoxyboric acid in a TEOS/trimethoxyboric acid weight
ratio of 10/3 are dissolved in ethanol, and the ethanol solution is coated on the
entire surface by a spin coating method at approximately 3000 rpm. Then, the
obtained supporting-member-forming film is subjected to temporary calcining or
sintering around 200 °C to remove an organic substance contained in the solution.
Further, the film is further subjected to main calcining or sintering around 500 °C
to give a state, by phase separation, where fine particles of boron oxide are
precipitated in a borosilicate glass. Then, etching with hot water is carried out,
whereby only the fine particles of boron oxide are dissolved and removed, and the
porous material member 45 composed of a borosilicate glass is obtained.
Procedure to come thereafter can be carried out in the same manner as in Example
3. In Example 4, the flat-panel display shown in Figs. 9 to 11 can be constituted
as well.
Example 5
-
Example 5 is another variant of Example 3. Example 5 differs
from Example 3 mainly in that the porous material member 45 is formed by
removing a component having a relatively high etching rate by etching. In the
step of forming the porous material member 45, first, for example, TEOS and
methyltrimethoxysilane in a TEOS/methyltrimethoxy silane weight ratio of 10/4
are dissolved in ethanol, and the ethanol solution is coated on the entire surface by
a spin coating method at approximately 3000 rpm. Then, the obtained supporting-member-forming
film is subjected to calcining or sintering around 200 °C to
remove an organic substance contained in the solution. In the supporting-member-forming
film obtained in this case, silicon oxide derived from TEOS and
silicon oxide derived from methyltrimethoxysilane are co-present. Then, etching
is carried out with a 1 % hydrofluoric acid aqueous solution, whereby the silicon
oxide derived from methyltrimethoxysilane having a relatively high etching rate is
removed by the etching, and the porous material member 45 of silicon oxide
derived from TEOS can be obtained. Procedure to come thereafter can be carried
out in the same manner as in Example 3. In Example 5, the flat-panel display
shown in Figs. 9 to 11 can be constituted as well.
Example 6
-
Example 6 is concerned with the production method according to
the second constitution of the present invention and the flat-panel display
according to the second constitution of the present invention obtained by the
above production method. Example 6 will be explained with reference to Figs.
12A, 12B, 13A and 13B hereinafter.
[Step-600]
-
Procedures up to the formation of an insulating layer 12 are carried
out in the same manner as in [Step-200] of Example 2. Then, a gate electrode 13
is formed on the insulating layer 12. The gate electrode 13 can be obtained by
forming the electrically conductive material layer 13' for a gate electrode and
patterning the electrically conductive material layer 13' by an etching method,
etc., as described in Example 2, or can be formed directly in the form of a stripe
by a screen-printing method. Then, an approximately 1 µm thick second
insulating layer 46 composed of SiO2 is formed on the gate electrode 13 and the
insulating layer 12, for example, by a CVD method. Further, an approximately
0.07 µm thick TiN layer is formed on the entire surface on the second insulating
layer 46 by a sputtering method, to form an electrically conductive material layer
for a focus electrode (electrically conductive material layer 47' for a focus
electrode). Further, a getter-forming layer 43 is formed on the electrically
conductive material layer 47' for a focus electrode in the same manner as in [Step-200]
of Example 2 (see Fig. 12A).
[Step-610]
-
Then, as shown in Fig. 12B, the getter-forming layer 43 and the
electrically conductive material layer 47' for a focus electrode are patterned,
whereby a focus electrode 47 having the second-type getter 43B formed on the
upper surface thereof can be formed. The patterning is carried out, for example,
by etching the getter-forming layer 43 and the electrically conductive material
layer 47' for a focus electrode through an etching mask (not shown).
[Step-620]
-
Then, as shown in Fig. 13A, the second insulating layer 46, the gate
electrode 13 and the insulating layer 12 are patterned, to form an opening portion
14 having the cathode electrode 11 exposed in a bottom portion thereof. The
opening portion 14 can be formed, for example, by etching the second insulating
layer 46, the gate electrode 13 and the insulating layer 12 through an etching mask
(not shown). In this case, the above patterning is carried out inside the opening
portion formed in the focus electrode 47, whereby an end portion of the focus
electrode 47 can be allowed to recede from the end portion of the gate electrode
13. The focus electrode 47 is originally provided to correct only the path of
electrons which deviate from the direction perpendicular to the cathode electrode
11 to a great extent, and when the opening diameter of the focus electrode 47 is
too small, the electron emission efficiency of the field emission device may
decrease. Particularly preferably, the end portion of the focus electrode 47
recedes from the end portion of the gate electrode 13 as described above, since the
necessary focusing effect alone can be produced without hindering the emission
of electrons.
[Step-630]
-
Then, steps similar to [Step-230] to [Step-250] of Example 2 are
carried out, to form a conical electron-emitting portion 15 in a portion of the
cathode electrode 11 which portion is positioned in a bottom portion of the
opening portion 14 and to allow a side wall surface of the opening portion 14
formed in the insulating layer 12 and the second insulating layer 46 to recede
under an isotropic etching condition, whereby a field emission device shown in
Fig. 13B can be completed. Further, a step similar to [Step-260] of Example 2 is
carried out, whereby a flat-panel display similar to one explained in Example 2
can be obtained in Example 6. In such a flat-panel display, the convergence of the
path of emitted electrons is improved and an optical crosstalk among the pixels is
therefore decreased, so that a higher fineness of a display screen can be attained
by more finely dividing each pixel. The second-type getter 43B may be replaced
with the first-type getter 43A or the third-type getter 43C.
Example 7
-
Example 7 is concerned with the production method according to
the third constitution of the present invention and the flat-panel display according
to the first constitution of the present invention obtained by the above production
method. Example 7 will be explained with reference to Figs. 14A and 14B below.
[Step-700]
-
Procedures up to the formation of the insulating layer 12 are carried
out in the same manner as in [Step-200] of Example 2. As shown in Fig. 14A,
then, a gate electrode 13 is formed on the insulating layer 12. The gate electrode
13 can be obtained by forming the electrically conductive material layer 13' for a
gate electrode and then patterning the electrically conductive material layer 13'
according to an etching method, etc., as described in Example 2, or it can be also
formed directly in the form of a stripe by a screen-printing method.
[Step-710]
-
As shown in Fig. 14B, then, the second-type getter 43B is formed
on the gate electrode 13. The second-type getter 43B may be formed by a method
in which the second-type getters 43B can be formed only on the gate electrodes 13
or by a method in which a getter-forming layer 43 is formed on the entire surface
and the getter-forming layer 43 is patterned. Since procedures thereafter can be
carried out in the same manner as in [Step-220] to [Step-260] of Example 2,
detailed explanations thereof are omitted. In Example 7, the flat-panel display
shown in Figs. 9 to 11 can be constituted as well.
-
Figs. 15A to 15C show three patterns of formed getters. Fig. 15A
shows a second-type getter 43B which is positioned on the gate electrode 13 and
extends onto the insulating layer 12. Fig. 15B shows a second-type getter 43B
which is positioned on an insulating layer 12 between one gate electrode 13 and
another gate electrode 13 which are adjacent to each other. Fig. 15C shows a
second-type getter 43B formed on the entire surface on the gate electrode 13 and
the insulating layer 12. As a getter, the second-type getter 43B may be replaced
with the first-type getter 43A or the third-type getter 43C. While the getter
pattern shown in Fig. 15C is a pattern which can give a maximum effective area
of the getter, the supporting member is required to have electrically insulating
properties for preventing short-circuiting between the adjacent gate electrodes 13.
The supporting member having electrically insulating properties includes a
structure constituted of an electrically insulating material layer; a polycrystalline
silicon layer and nearly hemispherical silicon particles; a porous material member
45 composed of an electrically insulating layer; and an electrically conductive
porous material member 45 formed on an electrically insulating material layer. In
the production method according to the third constitution of the present invention,
the gate electrode is formed in one step, and the getter is formed in another step,
so that it can be said that an example in which the pattern of the gate electrodes 13
and the pattern of the getters differ from each other more effectively utilizes the
characteristic of the production method according to the third constitution.
Example 8
-
Example 8 is concerned with the production method according to
the fourth constitution of the present invention and the flat-panel display
according to the second constitution of the present invention obtained by the
above production method. Only the difference of Example 8 from Example 6 will
be explained with reference to Figs. 16A and 16B.
[Step-800]
-
Procedures up to the formation of the second insulating layer 46 are
carried out in the same manner as in [Step-600] of Example 6. Then, a focus
electrode 47 is formed on the second insulating layer 46 (see Fig. 16A). The
focus electrode 47 can be obtained by forming the electrically conductive material
layer 47' for a focus electrode and then patterning the electrically conductive
material layer 47' by an etching method, etc., as described in Example 6, or it can
be also formed directly in the form of a stripe by a screen-printing method.
[Step-810]
-
As shown in Fig. 16B, then, the second-type getter 43B is formed
on the focus electrode 47. The second-type getter 43B can be formed by a method
in which the second-type getter 43B can be selectively formed on the focus
electrode 47 alone or by a method in which a getter-forming layer 43 is formed on
the entire surface and the getter-forming layer 43 is patterned. Since procedures
thereafter can be carried out in the same manner as in [Step-620] to [Step-630] of
Example 6, detailed explanations thereof are omitted. In Example 8, the flat-panel
display similar to that described in Example 6 can be constituted as well.
-
Figs. 17A to 17C show three patterns of formed getters. Fig. 17A
shows a second-type getter 43B which is positioned on the focus electrode 47 and
extends onto the second insulating layer 46. Fig. 17B shows a second-type getter
43B which is positioned on the second insulating layer 46 between one focus
electrode 47 and another focus electrode 47 which are adjacent to each other. Fig.
17C shows a second-type getter 43B formed on the entire surface on the focus
electrode 47 and the second insulating layer 46. As a getter, the second-type
getter 43B may be replaced with the first-type getter 43A or the third-type getter
43C. While the getter pattern shown in Fig. 17C is a pattern which can give a
maximum effective area of the getter, the supporting member is required to have
electrically insulating properties for preventing short-circuiting between the
adjacent focus electrodes 47. The supporting member having electrically
insulating properties includes a structure constituted of an electrically insulating
material layer; a polycrystalline silicon layer and nearly hemispherical silicon
particles; a porous material member 45 constituted of an electrically insulating
layer; and an electrically conductive porous material member 45 formed on an
electrically insulating material layer. In the production method according to the
fourth constitution of the present invention, the focus electrode 47 is formed in
one step, and the getter is formed in another step, so that it can be said that an
example in which the pattern of the focus electrodes 47 and the pattern of the
getters differ from each other more effectively utilizes the characteristic of the
production method according to the fourth constitution.
Example 9
-
Example 9 is concerned with the production method according to
the fifth constitution of the present invention and the flat-panel display according
to the third constitution of the present invention obtained by the above production
method. In Example 9, at least part of the gate electrode is composed of a gas-trapping
material. Specifically, Example 9 uses a zirconium-aluminum alloy (Zr-Al
alloy) as a gas-trapping material for constituting a gate electrode 113, and the
gate electrode 113 has a single-layered structure. Example 9 will be explained
with reference to Figs. 18A and 18B hereinafter.
[Step-900]
-
First, a cathode electrode 11 constituted of an electrically
conductive material layer of niobium (Nb) in the form of a stripe is formed on a
supporting substrate 10 made, for example, of glass, and an insulating layer 12
composed of SiO2 is formed on the entire surface. Further, the gate electrode 113
constituted of an electrically conductive material layer of a zirconium-aluminum
alloy (Zr-Al alloy) as a gas-trapping material in the form of a stripe is formed on
the insulating layer 12. The gate electrode 113 can be formed, for example, by a
sputtering method, lithography and a dry etching method. Then, an opening
portion 14 is formed in the gate electrode 113 and the insulating layer 12 by an
RIE (reactive ion-etching) method, to expose the cathode electrode 11 in a bottom
portion of the opening portion 14 (see Fig. 18A). The cathode electrode 11 may
be a single material layer, or it may be a stack of a plurality of material layers.
For suppressing the fluctuation of electron emission characteristics of the
electron-emitting portions to be formed at a step to come later, the surface layer
portion of the cathode electrode 11 can be composed of a material having a higher
electric resistivity than a material forming a remaining portion. Such a structure
of the cathode electrode can be applied to the field emission device in other
Examples.
[Step-910]
-
Thereafter, procedures in [Step-230] to [Step-250] in Example 2
are carried out, whereby a Spindt-type field emission device having a structure
shown in Fig. 18B can be completed.
-
Figs. 19A, 19B, 20A, 20B and 20C show variants of the gate
electrode.
-
The gate electrode shown in Fig. 19A does not have a single-layered
structure but has a stacked structure constituted of a first layer 113A
composed of an electrically conductive material such as nickel (Ni) and a second
layer 113B composed of a gas-trapping material. The first layer 113A may be
composed of an electrically insulating material such as a glass. In this case,
however, the second layer 113B is required to have electric conductivity.
-
The gate electrode shown in Fig. 19B has a stacked structure
constituted of a first layer 113A composed of an electrically conductive material
or a gas-trapping material, a second layer 113B composed of an electrically
insulating material and a third layer 113C composed of a gas-trapping material
(gas-trapping layer).
-
The gate electrode shown in Fig. 20A has a stacked structure
constituted of a first layer 113A composed of an electrically conductive material
and a second layer 113B composed of a gas-trapping material. Differing from the
gate electrode shown in Fig. 19A, the gate electrode has a structure in which the
upper end portion of the opening portion 14 formed in the first layer 113A has a
smaller opening size than the lower end portion thereof. When electrons emitted
from the electron-emitting portion 15 enters the insulating layer 12 near the first
layer 113A, gas may be released from such a portion of the insulating layer 12. In
the above structure, the risk of electrons colliding with the insulating layer 12
decreases even if the path of electrons curves toward the inner side wall of the
first layer 113A, so that the release of the gas from the insulating layer 12 can be
prevented.
-
The gate electrode shown in Fig. 20B also has a stacked structure
constituted of a first layer 113A composed of an electrically conductive material
and a second layer 113B composed of a gas-trapping material. Differing from the
gate electrode shown in Fig. 19A, the gate electrode has a structure in which the
upper end portion of the opening portion 14 formed in the first layer 113A has a
larger opening size than the lower end portion thereof.
-
The gate electrode shown in Fig. 20C also has a stacked structure
constituted of a first layer 113A composed of an electrically conductive material
and a second layer 113B composed of a gas-trapping material. Differing from the
gate electrode shown in Fig. 19A, the gate electrode has a structure in which the
upper end portion of the opening portion 14 formed in the first layer 113A has a
larger opening size than the lower end portion thereof and the opening end side
wall of the first layer 113A is covered with second layer 113B. In such a
structure, the opening end side wall of the opening portion 14 which serves as a
path of electrons in the gate electrode is brought into a state where the opening
end side wall is all covered with the second layer 113B composed of a gas-trapping
material, so that no gas is released from the gate electrode even if
electrons collide with the opening end side wall since a portion with which
electrons collide is necessarily composed of the gas-trapping material.
-
In the gate electrodes shown in Figs. 20A to 20C, a slanted opening
end side wall of the first layer 113A can be formed by optimizing a condition for
etching the first layer 113A.
-
The function of the gate electrode 113 produced by containing a
gas-trapping material will be explained more in detail below with reference to
Figs. 21A, 21B and 21C.
-
Fig. 21A shows an example of a pressure distribution when gas
molecules, etc., are released by the collision of electrons with the fluorescent layer
21 to increase a pressure up to approximately I Pa near the fluorescent layer 21.
Even when gas molecules, etc., are released near the fluorescent layer 21 to
increase the pressure, the released gas molecules, etc., are trapped by the gas-trapping
material of a gate electrode 113. Therefore, the pressure of the vacuum
layer decreases toward the electron-emitting portion 15, so that local discharging,
etc., which are involved in the releasing of the gas molecules, etc., is prevented,
and the detrimental effect on the electron-emitting portion 15 is prevented.
-
Fig. 21B shows an example of a pressure distribution near the
electron-emitting portion 15 when gas molecules, etc., released by the collision of
electrons with the fluorescent layer 21 reach the electron-emitting portion 15 to
cause gas molecules, etc., to be released from the electron-emitting portion 15.
Even when gas molecules, etc., are released in a site H1 near the electron-emitting
portion 15, the released gas molecules, etc., are trapped by the gas-trapping
material of the gate electrode 113. A pressure in the site H1 near the electron-emitting
portion 15, therefore, increases, for example, approximately by 2 x 10-4
Pa, and the pressure is not increased so high as to affect the electron-emitting
portion 15.
-
Fig. 21C shows an example of a pressure distribution when gas
molecules, etc., are released by the collision of electrons with the fluorescent layer
21 and further when gas molecules, etc., are released from the insulating layer 12
by the collision of electrons emitted from the electron-emitting portion and
distracted toward the insulating layer 12 with a wall surface H2 of the insulating
layer 12. Even if the gas molecules, etc., are released from the wall surface H2 of
the insulating layer 12, the released gas molecules, etc., are trapped by the gate
electrode 113, so that a pressure increases, for example, approximately by 2 x 10-3
Pa. Further, the pressure decreases toward the electron-emitting portion 15, and
the detrimental effect on the electron-emitting portion 15 is prevented.
Example 10
-
Example 10 is concerned with the production method according to
the sixth constitution of the present invention and the flat-panel display according
to the fourth constitution of the present invention obtained by the above
production method. In Example 10, at least part of the focus electrode is
composed of a gas-trapping material. Specifically, the gas-trapping material
constituting a focus electrode 147 is a zirconium-aluminum alloy (Zr-Al alloy),
and the focus electrode 147 has a single-layered structure. Example 10 will be
explained with reference to Figs. 22A and 22B hereinafter.
[Step-1000]
-
Procedures up to the formation of an insulating layer 12 are carried
out in the same manner as in [Step-200] of Example 2. Then, a gate electrode 13
is formed on the insulating layer 12. The gate electrode 13 can be obtained by
forming the electrically conductive material layer 13' for a gate electrode and then
patterning the electrically conductive material layer 13' according to an etching
method, etc., as described in Example 2, or it can be also formed directly in the
form of a stripe by a screen-printing method. Then, an approximately 1 µm thick
second insulating layer 46 composed of SiO2 is formed on the gate electrode 13
and the insulating layer 12, for example, by a CVD method. Further, the focus
electrode 147 composed of a zirconium-aluminum alloy (Zr-Al alloy) as a gas-trapping
material is formed in the form of a stripe on the second insulating layer
46. The focus electrode 147 can be formed, for example, by a sputtering method,
lithography or a dry etching method (see Fig. 22A).
[Step-1010]
-
Then, steps similar to [Step-620] to [Step-630] of Example 6 are
carried out, whereby a Spindt-type field emission device having a structure shown
in Fig. 22B can be completed.
-
The focus electrode 147 can be formed so as to have any one of
structures shown in Figs. 19A, 19B, 20A, 20B and 20C.
Example 11
-
Example 11 is concerned with the production method according to
the seventh constitution of the present invention and the flat-panel display
according to the fifth constitution of the present invention obtained by the above
production method. The field emission device of the flat-panel display of
Example 11 comprises:
- (A) a spacer 12 disposed on a supporting substrate 10 and
composed of an electrically insulating material,
- (B) a gate electrode 213 constituted of a gas-trapping material layer
213A which has a plurality of opening portions 214A formed therein and at least
part of which is composed of a gas-trapping material, and
- (C) an electron-emitting portion 15C formed on the supporting
substrate 10,
wherein the gas-trapping material layer 213A is fixed such that it
comes in contact with the top surface of the spacer 12 and that the opening portion
214A is positioned above the electron-emitting portion 15C.-
-
The gas-trapping material layer 213A is fixed to the top surface of
the spacer with a thermosetting adhesive (for example, an epoxy-containing
adhesive). Alternatively, as shown in Fig. 23 showing a schematic partial cross-sectional
view of an end portion of the supporting substrate 10, there may be
employed a structure in which each end portion of the gas-trapping material layer
213A in the form of a stripe is fixed to a circumferential portion of the supporting
substrate 10. More specifically, for example, projection portions 216 are formed
beforehand in the circumferential portion of the supporting substrate 10, a thin
film 217 composed of the same material as that used for constituting the gas-trapping
material layer 213A is formed on the top surface of the projection portion
216 beforehand, and the gas-trapping material layer 213A in the form of a stripe is
welded to the thin film 217 with a laser while it is in an expanded state. The
projection portion 216 can be formed concurrently with the formation of the
spacer.
-
As the gas-trapping material layer 213A in Example 11, a stacked
structure constituted of a first layer composed of nickel (Ni) as an electrically
conductive material and a second layer composed of a gas-trapping material is
used. The gas-trapping material layer 213A shall not be limited to the stacked
structure, and it may have a single-layered structure. In this case, examples of the
material for the gas-trapping material layer 213A include titanium (Ti), titanium
alloys such as a titanium-zirconium-vanadium-iron (Ti-Zr-V-Fe) alloy, carbon (C)
and barium (Ba). When a stacked structure is used as the gas-trapping material
layer 213A, it is preferred to form the second layer composed of a gas-trapping
material on the cathode electrode side, since a vacuum state around the cathode
electrode 211 can be maintained in a good condition. That is, it is preferred to
reverse the order of stacking of the first layer 113A and the second layer 113B in
the Figs. 19A, 20A, 20B and 20C.
-
In Example 11, a plane-type field emission device is used as a field
emission device. The plane-type field emission device comprises a cathode
electrode 211 formed in the form of a stripe on a supporting substrate 10 made,
for example, of a glass; an insulating layer 12 (corresponding to the spacer)
formed on the supporting substrate 10 and the cathode electrode 211; a gate
electrode 213 formed in the form of a stripe on the insulating layer 12; and an
opening portion 214 which is formed through the gate electrode 213 and the
insulating layer 12 and has the cathode electrode 211 exposed in the bottom
portion thereof. The cathode electrode 211 extends in the direction perpendicular
to the paper surface of Fig. 23, and the gate electrode 213 extends leftward and
rightward on the paper surface of Fig. 23. The cathode electrode 211 is composed
of chromium (Cr), and the insulating layer 12 is composed of SiO2. In this case,
that part of the cathode electrode 211 which is exposed in the bottom portion of
the opening portion 214 corresponds to an electron-emitting portion 15C and
corresponds to an electron-emitting layer.
-
One example of the method of producing the field emission device
in Example 11 will be explained below.
[Step-1100]
-
First, the cathode electrode 211 which works as an electron-emitting
portion 15C is formed on the supporting substrate 10. Specifically, an
electrically conductive material layer composed of chromium (Cr) for a cathode
electrode is formed on the supporting substrate 10 by a sputtering method, and the
electrically conductive material layer for a cathode electrode is patterned by
lithography and a dry etching method, whereby the cathode electrode 211
composed of the electrically conductive material layer in the form of a stripe can
be formed on the supporting substrate 10.
[Step-1110]
-
Then, an insulating layer 12 (corresponding to the spacer)
composed of SiO2 is formed on the entire surface, specifically, on the supporting
substrate 10 and the cathode electrode 211, by a CVD method. Alternatively, the
insulating layer 12 may be formed from a glass paste by a screen-printing method.
[Step-1120]
-
Then, the opening portion 214 is formed in the insulating layer 12
by lithography and an etching method. Otherwise, the opening portion 214 may
be formed together when the insulating layer 12 is formed by a screen-printing
method. In this manner, the surface of the cathode electrode 211 which surface
corresponds to the electron-emitting portion can be exposed in the bottom portion
of the opening portion 214. The insulating layer 12 corresponds to the spacer.
[Step-1130]
-
Then, the stripe-shaped gas-trapping material layer 213A having a
plurality of the opening portions 214A is disposed in a state in which it is
supported on the insulating layer 12 such that the opening portions 214A are
positioned above the electron-emitting portion and that the stripe-shaped gas-trapping
material layer 213A is disposed in a direction different from a direction
in which the cathode electrode 211 extends. In this manner, the gate electrode
213 which is constituted of the gas-trapping material layer 213A in the form of a
stripe and has a plurality of the opening portions 214A is positioned above the
electron-emitting portion.
-
A stripe-shaped material layer for a gate electrode 213 can be
prepared, for example, by the following method. That is, a nickel sheet for a first
layer 113A is provided, a gas-trapping material (such as titanium or a titanium-containing
alloy such as a titanium-zirconium-vanadium-iron alloy) is, for
example, applied to, or deposited on. the nickel sheet to form a second layer
113B. Then, the opening portions 214A having a predetermined form are formed
in the first layer 113A and the second layer 113B. There may be employed
procedures of forming the opening portions 214A in the first layer 113A in
advance and then forming the second layer 113B thereon. Preferably, the second
layer 113B is formed in a vacuum atmosphere or an atmosphere of an inert gas
such as argon (Ar) or helium (He) in order to prevent the second layer 113B from
trapping an unnecessary substance before the first panel P1 and the second panel
P2 are bonded.
-
The gas-trapping material layer 213A may be composed of a gas-trapping
material whose gas-trapping capability increases with an increase in
temperature, such as a zirconium-aluminum alloy or a titanium-zirconium-vanadium-iron
alloy. Fig. 24 shows a relationship between a temperature of a
zirconium-aluminum alloy (Al-Zr alloy) and a vacuuming rate in the internal
space of the flat-panel display. In Fig. 24, the axis of abscissas indicates
temperatures (°C), and the axis of ordinates indicates a vacuuming rate which is a
rate of the Al-Zr alloy trapping gas molecules, etc., in the internal space, and its
unit is ml/second•cm2. As is clearly shown in Fig. 24, the Al-Zr alloy has the
property of increasing its vacuuming rate with an increase in temperature (that is,
the gas-trapping capability thereof increases). Even if electrons emitted from the
electron-emitting portion 15C are curved toward the gate electrode 213 and
collide with the gate electrode 213 to cause the temperature increase of the gate
electrode 213, the Al-Zr alloy incorporated into the gate electrode 213 makes it
possible to expect an effect that the vacuuming rate in the gate electrode 213
increases, and the unstable performance caused on the flat-panel display by an
increase in temperature can be prevented. When it is intended to utilize the above
effect actively, preferably, not the first layer 113A but the second layer 113B has
such a form that electrons easily collide with it when the gate electrode 213 has a
stacked structure of the first layer 113A and the second layer 113B. When there is
employed a constitution in which the first layer 113A is covered with the second
layer 113B as shown in Fig. 20C, electrons inevitably enter the second layer
113B, and there can be expected the effect that the vacuuming rate is improved by
an increase in temperature. For activating the Al-Zr alloy to impart it with the
vacuuming function, it is at least required to heat the Al-Zr alloy to 300 °C or
higher. The activation is preferably carried out by heat treatment in a vacuum
atmosphere or an atmosphere of an inert gas such as argon or helium after the
formation of the gas-trapping material layer 213A but before [Step-1130]. The
above heat treatment can be carried out by irradiating the second layer 113B with
electron beam. Otherwise, it can be carried out by introducing the gas-trapping
material layer 213A into a generally employed high-temperature furnace.
-
The above method of forming the gate electrode can be applied to
the production of various field emission devices.
Example 12
-
Example 12 is a variant of Example 11. The field emission device
in Example 12 differs from the field emission device in Example 11 in that a rib
212 (corresponding to a spacer) is provided between one cathode electrode 211
and another cathode electrode 211 as is shown in a schematic partial cross-sectional
view of Fig. 25A. Fig. 25B shows a schematic layout of the cathode
electrodes 211, gas-trapping material layers 213A with the gate electrodes 213
and the ribs 212. When a stacked structure is employed as the gas-trapping
material layer 213A in the form of a stripe, preferably, the second layer composed
of the gas-trapping material is positioned on the cathode electrode side from the
viewpoint that the vacuum state around the cathode electrode 211 is maintained
under a good condition.
-
The gas-trapping material layer 213A is fixed to the top surface of
the ribs 212 with a thermosetting adhesive (for example, an epoxy-containing
adhesive). Otherwise, there may be employed a structure in which both ends of
the gas-trapping material layer 213A in the form of a stripe are fixed to the
circumferential portion of the supporting substrate 10 as shown in the schematic
partial cross-sectional view of Fig. 23. More specifically, projection portions 216
are formed in the circumferential portion of the supporting substrate 10
beforehand, and a thin film 217 composed of the same material as that used for
the gas-trapping material layer 213A is formed on the top surface of the projection
portion 216 beforehand. While the gas-trapping material layer 213A in the form
of a stripe is in an expanded state, the gas-trapping material layer 213A is welded
to the thin film 217, for example, with a laser.
-
The field emission device in Example 12 can be prepared, for
example, by the following method.
[Step-1200]
-
The rib 212 constituting a spacer (gate electrode support) in the
form of a stripe is formed on the supporting substrate 10, for example, by a
sandblasting method.
[Step-1210]
-
Then. an electron-emitting portion is formed on the supporting
substrate 10. Specifically, a mask layer composed of a resist material is formed
on the entire surface by a spin coating method, and the mask layer is removed
from a region where the cathode electrode is to be formed and which is between
one rib 212 and another rib 212. Then, an electrically conductive material layer
composed of chromium (Cr) for a cathode electrode is formed on the entire
surface by a sputtering method in the same manner as in [Step-1100], and then the
mask layer is removed, whereby the electrically conductive material layer formed
on the mask layer is also removed and the cathode electrode 211 which works as
an electron-emitting portion is retained between one rib 212 and another rib 212.
[Step-1220]
-
The stripe-shaped gas-trapping material layer 213A having a
plurality of the opening portions 214A is disposed in a state in which it is
supported on the ribs 212, which are the spacers, such that a plurality of the
opening portions 214A are positioned above the electron-emitting portion,
whereby the gate electrode 213 which is constituted of the gas-trapping material
layer 213A in the form of a stripe and has a plurality of the opening portions 214A
is positioned above the electron-emitting portion. The gas-trapping material layer
213A in the form of a stripe can be arranged as described above.
-
The above method of forming the gate electrode can be applied to
the production of various field emission devices.
-
In the field emission device in Example 11 or 12, the plane form of
the opening portions 214A is not limited to a circular form. Figs. 26A, 26B, 26C
and 26D show variants of the form of the opening portions 214A formed in the
gas-trapping material layer 213A.
Example 13
-
Examples 13 to 27 will explain field emission devices having
various constitutions and structures and methods for the production thereof. All
of these field emission devices can be applied to the flat-panel displays explained
in Examples 1 to 12. That is, all of the gate electrode and the getter in the field
emission device constituting the flat-panel display according to the first
constitution and the gate electrode in the field emission device constituting the
flat-panel displays according to the third and fifth constitutions can be applied to
Examples 13 to 27. The above gate electrode/getter or the above gate electrode
will be expressed as a gate electrode 313 or 313B and is indicated by such a
reference numeral in Figures. The gate electrode 313 or 313B can be formed and
produced according to any method explained in Examples 1 to 12. Further,
Examples 13 to 27 may use the focus electrode explained in any one of Examples
6, 8 and 10.
-
In addition to the foregoing Spindt type field emission device (a
conical electron-emitting portion is formed on that portion of a cathode electrode
which is positioned in the bottom portion of an opening portion), the field
emission device includes a crown-type field emission device (a crown-shaped
electron-emitting portion is formed on that portion of a cathode electrode which is
positioned in the bottom portion of an opening portion), a flat-type field emission
device (a nearly flat electron-emitting portion is formed on that portion of a
cathode electrode which is positioned in the bottom portion of an opening
portion), a plane-type field emission device which is for emitting electrons from a
flat surface of a cathode electrode, a crater-type field emission device which is for
emitting electrons from a convex portion of surface of a cathode electrode having
a convexo-concave surface, and an edge-type field emission device.
-
First, the crown-type field emission device and the method of
producing the same will be explained below.
-
Fig. 29A shows a schematic partial end view of the crown-type
field emission device, and Fig. 29B shows a partially cut-out schematic
perspective view thereof. The crown-type field emission device comprises a
cathode electrode II formed on a supporting substrate 10; an insulating layer 12
formed on the supporting substrate 10 and the cathode electrode 11; a gate
electrode 313 formed on the insulating layer 12; an opening portion 14 which
penetrates through the gate electrode 313 and is formed in the insulating layer 12;
and a crown-type electron-emitting portion 15A in a portion of the cathode
electrode 11 which portion is positioned in a bottom portion of the opening
portion 14.
-
The method of producing the crown-type field emission device will
be explained below with reference to Figs. 27A, 27B, 28A, 28B, 28C, 28D, 29A
and 29B showing schematic partial end views, etc., of the supporting substrate
and the like.
[Step-1300]
-
First, the cathode electrode 11 constituted of an electrically
conductive material layer for a cathode electrode in the form of a stripe is formed
on the supporting substrate 10 made, for example, of a glass. The cathode
electrode 11 extends leftward and rightward on a paper surface of drawings. The
electrically conductive material layer for a cathode electrode in the form of a
stripe can be obtained, for example, by forming an approximately 0.2 µm thick
ITO film on the entire surface of the supporting substrate 10 and then patterning
the ITO film. The cathode electrode 11 can be a single material layer or a stacked
structure constituted of a plurality of material layers. For example, for
suppressing the fluctuation of electron emission characteristics of the electron-emitting
portions to be formed at a step to come later, the surface layer portion of
the cathode electrode 11 may be composed of a material having a higher electric
resistivity than a material constituting a remaining portion. Then, the insulating
layer 12 is formed on the entire surface, specifically, on the supporting substrate
10 and the cathode electrode 11. In this embodiment, for example, a glass paste
having a thickness of approximately 3 µm is screen-printed on the entire surface.
Then, for removing water and a solvent contained in the insulating layer 12 and
flattening the insulating layer 12, two-stage calcining or sintering procedures such
as temporary calcining or sintering at 100 °C for 10 minutes and main calcining or
sintering at 500 °C for 20 minutes are carried out. The above screen-printing
using a glass paste may be replaced with the formation of an SiO2 film, for
example, by a CVD method.
-
Then, the gate electrode 313 is formed on the insulating layer 12
(see Fig. 27A). The gate electrode 313 is extending in the direction perpendicular
to the paper surface of drawings. The material for the gate electrode 313 can be
selected from those explained in the foregoing Spindt-type field emission device.
The extending direction of projection image of the gate electrode 313 forms an
angle of 90° with the extending direction of projection image of the cathode
electrode 11 in the form of a stripe.
[Step-1310]
-
The gate electrode 313 and the insulating layer 12 are etched
through an etching mask EM composed, for example, of a photoresist material
according to an RIE method, to form an opening portion 14 through the gate
electrode 313 and the insulating layer 12 and to expose the cathode electrode 11 in
the bottom portion of the opening portion 14 (see Fig. 27B). The opening portion
14 has a diameter of approximately 2 to 50µm.
[Step-1320]
-
Then, the etching mask EM is removed, and a peel layer 51 is
formed on the gate electrode 313, the insulating layer 12 and the side wall surface
of the opening portion 14 (see Fig. 28A). The above peel layer 51 is formed, for
example, by applying a photoresist material onto the entire surface by a spin
coating method and patterning the photoresist material layer such that only part on
the bottom portion of the opening portion 14 is removed. At this stage, the
diameter of the opening portion 14 is substantially decreased to approximately 1
to 20 µm.
[Step-1330]
-
Then, as shown in Fig. 28B, an electrically conductive composition
layer 52 composed of a composition material is formed on the entire surface. The
above composition material contains, for example, 60 % by weight of graphite
particles having an average particle diameter of approximately 0.1 µm as
electrically conductive particles and 40 % by weight of No. 4 water glass as a
binder. The composition material is spin coated on the entire surface, for
example, at 1400 rpm for 10 seconds. The surface of the electrically conductive
composition layer 52 in the opening portion 14 rises along the side wall surface of
the opening portion 14 and dents toward the central portion of the opening portion
14 due to the surface tension of the composition material. Then, temporary
calcining or sintering for removing water contained in the electrically conductive
composition layer 52 is carried out, for example, in atmosphere at 400 °C for 30
minutes.
-
In the composition material, (1) the binder may be a dispersing
medium which forms a dispersion for the electrically conductive particles in itself,
or (2) the binder may coat each electrically conductive particle, or (3) the binder
may constitute a dispersing medium for the electrically conductive particles when
the binder is dispersed or dissolved in a proper solvent. A typical example of the
above case (3) is water glass, and the water glass can be selected from Nos. 1 to 4
defined under Japan Industrial Standard (JIS) K1408 or products equivalent
thereto. Nos. 1 to 4 refer to four grades based on different molar amounts
(approximately 2 to 4 mols) of silicon oxide (SiO2) per one mol of sodium oxide
(Na2O) which components of water glass, and differ from one another in
viscosity. When water glass is used in a lift-off process, therefore, it is preferred
to select an optimum water glass while taking into account various conditions
such as a kind and a content of the electrically conductive particles to be dispersed
in water glass, affinity to the peel layer 51, an aspect ratio of the opening portion
14, and the like, or it is preferred to prepare water glass equivalent to such a grade
before use.
-
The binder is generally poor in electric conductivity. When the
content of the binder is too large relative to the content of the electrically
conductive particles in the electrically conductive composition, therefore, the
electron-emitting portion 15A formed may show an increase in electric resistance
value, and electron emission may not proceed smoothly. For example, in a
composition material which is a dispersion of carbon-containing material particles
as electrically conductive particles in water glass, the content of the carbon-containing
material particles based on the total amount of the composition
material is preferably determined to be in the range of approximately 30 to 95 %
by weight while taking into account properties such as an electric resistance value
of the electron-emitting portion 15A, a viscosity of the composition material and
mutual adhesion of the electrically conductive particles. When the content of the
carbon-containing material particles is selected from the above range, the electric
resistance value of the electron-emitting portion 15A formed can be sufficiently
decreased, and the mutual adhesion of the carbon-containing material particles can
be maintained under a good condition. However, when a mixture of carbon-containing
material particles with alumina particles is used as electrically
conductive particles, the mutual adhesion of the electrically conductive particles is
liable to decrease, so that it is preferred to increase the content of the carbon-containing
material particles depending upon the content of the alumina particles.
The content of the carbon-containing material particles is particularly preferably
60 % by weight or more. The composition material may contain a dispersing
agent for stabilizing the dispersing state of the electrically conductive particles
and additives such as a pH adjuster, a desiccant, a curing agent and an antisepatic.
There may be used a composition material prepared by coating the electrically
conductive particles with a binder to prepare a powder and dispersing the powder
in a proper dispersing medium.
-
For example, when the crown-shaped electron-emitting portion
15A has a diameter of approximately 1 to 20 µm and when carbon-containing
material particles are used as electrically conductive particles, preferably, the
particle diameter of the carbon-containing material particles is approximately in
the range of from 0.1 µm to 1 µm. When the particle diameter of the carbon-containing
material particles is in the above range, an edge portion of the crown-shaped
electron-emitting portion 15A is imparted with sufficiently high
mechanical strength, and the adhesion of the electron-emitting portion 15A to the
cathode electrode 11 comes to be excellent.
[Step-1340]
-
Then, as shown in Fig. 28C, the peel layer 51 is removed. The
peeling is carried out by immersion in a sodium hydroxide aqueous solution of 2
% by weight for 30 seconds. The peeling may be carried out under supersonic
vibration. In this manner. the peel layer 51 and part of the electrically conductive
composition layer 52 on the peel layer 51 are together removed, and only that
portion of the electrically conductive material layer 52 which is on the exposed
cathode electrode 11 in the bottom portion of the opening portion 14 remains.
The above remaining portion constitutes the electron-emitting portion 15A. The
electron-emitting portion 15A has a surface denting toward the central portion of
the opening portion 14 and comes to have the form of a crown. Figs. 29A and
29B schematically show a state after [Step-1340] is finished. Fig. 29B is a
schematic perspective view of part of the field emission device, and Fig. 29A is a
schematic partial end view taken along line A-A in Fig. 29B. In Fig. 29B, part of
the insulating layer 12 and part of the gate electrode 313 are cut out for showing
the whole of the electron-emitting portion 15A. It is sufficient to form
approximately 5 to 100 electron-emitting portions 15A in one electron-emitting
region (overlap region). For reliably exposing the electrically conductive particles
on the surface of each electron-emitting portion 15A, a binder exposed on the
surface of each electron-emitting portion 15A may be removed by etching.
[Ste-1350]
-
Then, the electron-emitting portion 15A is calcined or sintered.
The calcining or sintering is carried out in dry atmosphere at 400 °C for 30
minutes. The calcining or sintering temperature can be selected depending upon
the binder contained in the composition material. For example, when the binder is
an organic material such as water glass, it is sufficient to carry out heat treatment
at a temperature at which the inorganic material can be calcined or sintered.
When the binder is a thermosetting resin, the heat treatment can be carried out at a
temperature at which the thermosetting resin can be cured. For maintaining
mutual adhesion of the electrically conductive particles, however, the heat
treatment is preferably carried out at a temperature at which the thermosetting
resin is neither decomposed to excess nor carbonized. In either case, the heat
treatment temperature is required to be a temperature at which neither damage nor
a defect is caused on the gate electrode, the cathode electrode and the insulating
layer. The heat treatment atmosphere is preferably an inert gas atmosphere for
preventing an oxidation from causing an increase in the electric resistivity of the
gate electrode and the cathode electrode and for preventing the gate electrode and
the cathode electrode from suffering damage or defects. When a thermoplastic
resin is used as a binder, no heat treatment may be required in some case.
Example 14
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Fig. 30C shows a schematic partial cross-sectional view of a tlat-type
field emission device. The flat-type field emission device comprises a
cathode electrode 11 formed on a supporting substrate 10 made, for example, of a
glass; an insulating layer 12 formed on the supporting substrate 10 and the
cathode electrode 11; a gate electrode 313 formed on the insulating layer 12; an
opening portion 14 which penetrates through the gate electrode 313 and is formed
in the insulating layer 12; and a flat electron-emitting portion 15B formed on a
portion of the cathode electrode 11 which portion is positioned in the bottom
portion of the opening portion 14. The electron-emitting portion 15B is formed
on the cathode electrode 11 in the form of a stripe extending in the direction
perpendicular to the paper surface of Fig. 30C. Further, the gate electrode 313 is
extending leftward and rightward on the paper surface of Fig. 30C. The cathode
electrode 11 and the gate electrode 313 are composed of chromium (Cr).
Specifically, the electron-emitting portion 15B is constituted of a thin layer
composed of a graphite powder. A resistance layer 60 composed of SiC is formed
between the cathode electrode 11 and the electron-emitting portion 15B for
stabilizing the performance of the field emission device and attaining uniform
electron emission characteristics. In the flat-type field emission device shown in
Fig. 30C, the resistance layer 60 and the electron-emitting portion 15B are formed
all over the surface of the cathode electrode 11. However, the present invention
shall not be limited to such a structure, and it is sufficient to form the electron-emitting
portion 15B at least in the bottom portion of the opening portion 14.
The method of producing the flat-type field emission device will be
explained hereinafter with reference to Figs. 30A, 30B and 30C showing the
schematic partial cross-sectional views of the supporting substrate, etc.
[Step-1400]
-
An electrically conductive material layer composed of chromium
(Cr) for a cathode electrode is formed on the supporting substrate 10 by a
sputtering method and patterned by lithography and a dry etching method,
whereby the cathode electrode 11 composed of the electrically conductive
material layer in the form of a stripe can be formed on the supporting substrate 10
(see Fig. 30A). The cathode electrode 11 is extending in the direction
perpendicular to the paper surface of Fig. 30A.
[Step-1410]
-
Then, the electron-emitting portion 15B is formed on the cathode
electrode 11. Specifically, the resistance layer 60 composed of SiC is formed on
the entire surface by a sputtering method. Then, the electron-emitting portion 15B
composed of a graphite powder coating is formed on the resistance layer 60 by a
spin coating method and is dried. Then, the electron-emitting portion 15B and the
resistance layer 60 are patterned by a known method (see Fig. 30B). The
electron-emitting portion 15B is to emit electrons.
[Step-1420]
-
Then, the insulating layer 12 is formed on the entire surface.
Specifically, the insulating layer 12 composed of SiO2 is formed on the electron-emitting
portion 15B and the supporting substrate 10, for example, by a sputtering
method. Alternatively, the insulating layer 12 may be formed by a method in
which a glass paste is screen-printed or by a method in which a layer of SiO2 is
formed by a CVD method. Then, the gate electrode 313 in the form of a stripe is
formed on the insulating layer 12.
[Step-1430]
-
The opening portion 14 is formed through the gate electrode 313
and the insulating layer 12 to expose the electron-emitting portion 15B in the
bottom portion of the opening portion 14. Then, heat treatment is carried out at
400 °C for 30 minutes for removing an organic solvent in the electron-emitting
portion 15B, whereby the field emission device shown in Fig. 30C can be
obtained.
Example 15
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Example 15 is a variant of Example 14. Fig. 31C shows a
schematic partial cross-sectional view of the flat-type field emission device in
Example 15. The flat-type field emission device shown in Fig. 31C differs from
the flat-type field emission device shown in Fig. 30C in the structure of the
electron-emitting portion 15B to some extent. The method of producing such a
field emission device will be explained below with reference to Figs. 31A, 31B
and 31C showing schematic partial cross-sectional views of a supporting
substrate, etc.
[Step-1500]
-
First, the electrically conductive material layer for a cathode
electrode is formed on the supporting substrate 10. Specifically, a resist material
layer (not shown) is formed on the entire surface of the supporting substrate 10,
and the resist material layer is removed from a portion where the cathode
electrode is to be formed. Then, the electrically conductive material layer
composed of chromium (Cr) for a cathode electrode is formed on the entire
surface by a sputtering method. Further, the resistance layer 60 composed of SiC
is formed on the entire surface by a sputtering method, and a graphite powder
coating layer is formed on the resistance layer 60 by a spin coating method and is
dried. Then, the resist material layer is removed with a peeling solution. In this
case, the electrically conductive material layer for a cathode electrode, the
resistance layer 60 and the graphite powder coating layer, which are formed on
the resist material layer, are also removed. In this manner, a structure in which
the cathode electrode 11, the resistance layer 60 and the electron-emitting portion
15B are stacked can be obtained according to a so-called lift-off method (see Fig.
31A).
[Step-1510]
-
Then. the insulating layer 12 is formed on the entire surface, and
the gate electrode 313 in the form of a stripe is formed on the insulating layer 12
(see Fig. 31B). Then, the opening portion 14 is formed through the gate electrode
313 and the insulating layer 12 to expose the electron-emitting portion 15B in the
bottom portion of the opening portion 14 (see Fig. 31C). Electrons are to be
emitted from the electron-emitting portion 15B formed on the surface of the
cathode electrode 11 which surface is exposed in the bottom portion of the
opening portion 14.
Example 16
-
Example 16 is a variant of the plane-type field emission device
explained in Example 11. The plane-type field emission device of which the
schematic partial cross-sectional view is shown in Fig. 32A differs from the
plane-type field emission device shown in Fig. 23 in that a fine convexo-concave
portion 11A is formed on that surface (corresponding to an electron-emitting
portion 15C) of a cathode electrode 211 which is exposed in the bottom portion of
the opening portion 14. Such a plane-type field emission device can be produced
by the following production method.
[Step-1600]
-
First, a cathode electrode 211 (electron-emitting layer) which
works as the electron-emitting portion 15C is formed on a supporting substrate 10.
Specifically, an electrically conductive material layer composed of tungsten (W)
for a cathode electrode is formed on the supporting substrate 10 by a sputtering
method, and the electrically conductive material layer for a cathode electrode is
patterned by lithography and a dry etching method, whereby the cathode electrode
211 constituted of the electrically conductive material layer for a cathode
electrode in the form of a stripe can be formed on the supporting substrate 10.
[Step-1610]
-
Then, an insulating layer 12 composed of SiO2 is formed on the
entire surface, specifically, on the supporting substrate 10 and the cathode
electrode 211, for example, by a CVD method. The insulating layer 12 may be
formed from a glass paste by a screen-printing method. In this case, the opening
portion 14 may be concurrently formed.
[Step-1620]
-
Then, a gate electrode 313 is formed on the insulating layer 12.
[Step-1630]
-
Then, the opening portion 14 is formed in the gate electrode 313
and the insulating layer 12 by lithography and an etching method to expose the
cathode electrode 211 in the bottom portion of the opening portion 14. In this
manner, the surface of the cathode electrode 211 which surface corresponds to an
electron-emitting portion can be exposed in the bottom portion of the opening
portion 14. Then, a fine convexo-concave portion 11A is formed on a portion of
the cathode electrode which portion is exposed in the bottom portion of the
opening portion 14. When the fine convexo-concave portion 11A is formed, and
drying etching using SF6 as an etching gas is carried out by an RIE method under
a condition where an etching rate of grain boundaries comes to be greater than
that of tungsten particles constituting the cathode electrode 211. As a result, the
fine convexo-concave portion 11A having dimensions nearly reflecting grain
diameters of the tungsten crystals can be formed.
-
In the above plane-type field emission device, an intense electric
field from the gate electrode 313 is applied to the tine convexo-concave portion
11A of the cathode electrode 211. more specifically to convex portions of the fine
convexo-concave portion 11A. In this case, the electric filed applied on the
convex portions is intense as compared with a case where the surface of the
cathode electrode 211 is flat and smooth, so that electrons are efficiently emitted
from the convex portions due to a quantum tunnel effect. It can be therefore
expected that the flat-panel display into which the above plane-type field emission
devices are incorporated is improved in brightness as compared with the plane-type
field emission device having a simply flat and smooth cathode electrode 211
exposed in the bottom portion of the opening portion 14. in the plane-type field
emission device shown in Fig. 32A, therefore, a sufficient current density of
emitted electrons can be obtained even if the potential difference between the gate
electrode 313 and the cathode electrode 211 is relatively small, and a higher
brightness of the flat-panel display can be achieved. In other words, the gate
voltage required can be decreased if the levels of the brightness are the same, and
the power consumption can be lowered.
-
In the above-explained embodiment, the opening portion 14 is
formed by etching the insulating layer 12 and then the fine convexo-concave
portion 11A is formed in the cathode electrode 211 by an anisotropic etching
method. However, the fine convexo-concave portion 11A can be also
simultaneously formed by the etching which is carried out for forming the
opening portion 14. That is, when the insulating layer 12 is etched, an anisotropic
etching condition which is expected to have ion-sputtering functions in some
extent is employed, and the etching is continued until after the opening portion 14
having a perpendicular wall is formed, whereby the fine convexo-concave portion
11A can be formed in that portion of the cathode electrode 211 which is exposed
in the bottom portion of the opening portion 14. Then, the insulating layer 12 can
be isotropically etched.
-
In a step similar to [Step-1600], an electrically conductive material
layer composed of tungsten for a cathode electrode is formed on the supporting
substrate 10 by a sputtering method, and then, the electrically conductive material
layer is patterned by lithography and a dry etching method. Then, the fine
convexo-concave portion 11A is formed on a surface of the electrically
conductive material layer for a cathode electrode, and steps similar to the steps
after [Step-1610] are carried out, whereby an field emission device similar to one
shown in Fig. 32A can be produced.
-
Otherwise, in a step similar to [Step-1600], the electrically
conductive material layer composed of tungsten for a cathode electrode is formed
on the supporting substrate 10 by a sputtering method, and then, the fine convexo-concave
portion 11A is formed in a surface of the electrically conductive material
layer for a cathode electrode. Then, the electrically conductive material layer is
patterned by lithography and a dry etching method, and steps similar to the steps
after [Step-1610] are carried out, whereby an field emission device similar to one
shown in Fig. 32A can be produced.
-
Fig. 32B shows a variant of the field emission device shown in Fig.
32A. In the field emission device shown in Fig. 32B, the average height position
of peaks of the fine convexo-concave portion 11A is present at a level lower than
the lower surface of the insulating layer 12 on the supporting substrate side (that
is, lowered). For producing such an field emission device, the dry etching in a
step similar to [Step-1600] can be continued for a longer period of time. In such a
constitution, the electric field intensity near the central portion of the opening
portion 14 can be further increased.
-
Fig. 33 shows a plane-type field emission device in which a coating
layer 11 B is formed on the surface of the cathode electrode 11 corresponding to
the electron-emitting portion 15C (more specifically, at least on the fine convexo-concave
portion 11A).
-
Preferably, the above coating layer 11B is composed of a material
having a smaller work function ( than a material constituting the cathode electrode
211. The material for the coating layer 11B can be determined depending upon
the work function of a material constituting the cathode electrode 211, a potential
difference between the gate electrode 313 and the cathode electrode 211 and the
current density of emitted electrons to be required. The material for the coating
layer llB includes amorphous diamond. When the coating layer 11B is
composed of amorphous diamond, the current density of emitted electrons
required for a flat-panel display can be obtained at an electric field of 5 x 107 V/m
or less.
-
The thickness of the coating layer 11B is determined to such an
extent that the coating layer 11B can reflect the fine convexo-concave portion
11A. That is because it is meaningless to form the fine convexo-concave portion
11A if the concave portions of the fine convexo-concave portion 11A are filled
with the coating layer 11B to flatten the surface of the electron-emitting portion.
Therefore, when. for example, the fine convexo-concave portion 11A is formed
while reflecting crystal grain diameters of the electron-emitting portion, the
thickness of the coating layer 11B is approximately 30 to 100 nm, although the
thickness differs depending upon dimensions of the fine convexo-concave portion
11A. When the average height position of peaks of the fine convexo-concave
portion 11A is lowered to a level below the lower surface position of the
insulating layer 12, to be exact, it is more preferred to lower the average height
position of peaks of the coating layer 11B to a level below the lower surface
position of the insulating layer 12.
-
Specifically, after [Step-1630], the coating layer 11B composed of
amorphous diamond can be formed on the entire surface, for example, by a CVD
method. The coating layer 11B is also deposited on an etching mask (not shown)
formed on the gate electrode 313 and the insulating layer 12. This deposit portion
is removed concurrently with the removal of the etching mask. The coating layer
11B can be formed by a CVD method using, for example, CH4/H2 mixed gases or
CO/H2 mixed gases as a source gas, and the coating layer 11B composed of
amorphous diamond is formed by thermal decomposition of the gas containing
carbon.
-
Otherwise, the field emission device shown in Fig. 33 can be
formed as follows. In a step similar to [Step-1600], an electrically conductive
material layer composed of tungsten for a cathode electrode is formed on the
supporting substrate 10 by a sputtering method, then, the electrically conductive
material layer is patterned by lithography and a dry etching method, and then, the
fine convexo-concave portion 11A is formed on a surface of the electrically
conductive material layer. Then, the coating layer 11B is formed, and then,
procedures after [Step-1610] are carried out.
-
Otherwise, the field emission device shown in Fig. 33 can be
produced as follows. In a step similar to [Step-1600], an electrically conductive
material layer composed of tungsten for a cathode electrode is formed on the
supporting substrate 10 by a sputtering method, then, the fine convexo-concave
portion 11A is formed on a surface of the electrically conductive material layer,
and then, the coating layer 11B is formed. Then, the coating layer 11B and the
electrically conductive material layer are patterned by lithography and a dry
etching method, and procedures after [Step-1610] are carried out.
-
Otherwise, the material for the coating layer can be selected from
materials which have a larger secondary electron gain δ than an electrically
conductive material which is to constitute the cathode electrode.
-
A coating layer may be formed on the electron-emitting portion
15C (on the surface of the cathode electrode 211) of the plane-type field emission
device shown in Fig. 23. In this case, after [Step-1120], the coating layer 11B can
be formed on the surface of the cathode electrode 211 which surface is exposed in
the bottom portion of the opening portion 14. Otherwise, in [Step-1100], for
example, an electrically conductive material layer for a cathode electrode is
formed on the supporting substrate 10, the coating layer 11B is formed on the
electrically conductive material layer, and these layers are patterned by
lithography and a dry etching method.
Example 17
-
Fig. 37B shows a schematic partial cross-sectional view of the
crater-type field emission device. In the crater-type field emission device, a
cathode electrode 411 having a plurality of projection portions 411A for emitting
electrons and concave portions 411B each of which is surrounded by the
projection portion 411A is provided on the supporting substrate 10. Fig. 36B
shows a schematic perspective view of the crater-type field emission device from
which an insulating layer 12 and a gate electrode 313 are removed.
-
While the form of each concave portion is not specially limited,
each concave portion has a nearly spherical surface, which is related to the
following fact. In the production of the above crater-type field emission device.
spheres are used, and part of each sphere is reflected when each concave portion
411B is formed. When each concave portion 411B has a nearly spherical surface,
the projection portion 411A surrounding the concave portion 411B is ringed or
circular, and in this case, the concave portion 411B and the projection portion
411A as a whole have a crater-like or caldera-like form. The projection portion
411A is for emitting electrons, so that a top end portion 411C of each particularly
preferably is sharp in view of improving electron emission efficiency. The profile
of top end portion 411C of each projection portion 411 A may have an irregular
convexo-concave form or may be flat. The layout of the projection portions 411 A
per pixel may be regular or at random. Each concave portion 411B may be
surrounded by the projection portion 411A continued along the circumferential
direction of the concave portion 411 A, and in some cases, each concave portion
411B may be surrounded by the projection portion 411A discontinuous along the
circumferential direction of the concave portion 411B.
-
In the method of producing the above crater-type field emission
device, more specifically, the step of forming the cathode electrode in the form of
a stripe on the supporting substrate comprises the steps of forming an electrically
conductive material layer for a cathode electrode in the form of a stripe on the
supporting substrate, such that the electrically conductive material layer covers a
plurality of spheres; and removing the spheres to remove a portion of the
electrically conductive material layer for a cathode electrode which portion covers
the sphere and thereby forming a cathode electrode having a plurality of
projection portions for emitting electrons and concave portions each of which is
surrounded by the projection portion and reflects part of the sphere.
-
Preferably, the spheres are removed by state change and/or
chemical change of the spheres. The state change and/or chemical change of the
sphere includes changes such as expansion, sublimation, foaming, gas generation,
decomposition, combustion and carbonization and combinations of these. For
example, when the spheres are composed of an organic material, more preferably,
the spheres are removed by combustion. The removal of the spheres and the
removal of portion of the electrically conductive material layer for a cathode
electrode which portion covers the sphere are not necessarily required to take
place concurrently, or the removal of the spheres and the removal of portions of
the electrically conductive material layer for a cathode electrode, the insulating
layer and the gate-electrode-constituting layer which portions cover the sphere are
not necessarily required to take place concurrently. For example, when part of the
spheres remain after the portion of the electrically conductive material layer for a
cathode electrode which portion covers the sphere or when the above portion and
the portions of the insulating layer and the gate-electrode-constituting layer are
removed, the remaining spheres can be removed later.
-
In particular, when the spheres are composed of an organic material
and when the spheres are combusted, for example, carbon monoxide, carbon
dioxide and vapor steam are generated to increase a pressure in a closed space
near the sphere, and the electrically conductive material layer for a cathode
electrode near the sphere bursts when a pressure durability limit is exceeded. The
portion of the electrically conductive material layer for a cathode electrode which
portion covers the sphere is dissipated by the force of the burst, to form the
projection portion and the concave portion, and the sphere is also removed.
Otherwise, when the spheres are, for example, combusted, the electrically
conductive material layer for a cathode electrode, the insulating layer and the
gate-electrode-constituting layer burst according to a similar mechanism when a
pressure durability limit is exceeded. Portions of the electrically conductive
material layer for a cathode electrode, the insulating layer and the gate-electrode-constituting
layer are dissipated by the force of the burst, to form the projection
portion and the concave portion and to form the opening portion at the same time,
and the sphere is also removed. That is, no opening portion exists in the
insulating layer and the gate-electrode-constituting layer before the removal of the
spheres, and the opening portion is formed together with the removal of the
sphere. In this case, the initial process of combustion proceeds in a closed space,
so that part of the spheres may be carbonized. Preferably, the thickness of portion
of the electrically conductive material layer for a cathode electrode which portion
covers the sphere is decreased to such an extent that said portion can be dissipated
by the burst. Otherwise, preferably, the thickness of each of portions of the
electrically conductive material layer for a cathode electrode, the insulating layer
and the gate-electrode-constituting layer which portions cover the sphere is
decreased to such an extent that said portions can be dissipated by the burst. In
the insulating layer, particularly preferably, its portion covering no spheres has a
thickness nearly equal to a diameter of each sphere.
-
In an field emission device in Example 19 to be described later, the
spheres can be removed by state change and/or chemical change of the spheres.
Since, however, the bursting of the electrically conductive material layer for a
cathode electrode is not involved, the spheres can be easily removed by exerting
an external force in some cases. In an field emission device in Example 20 to be
described later, the opening portion is formed prior to the removal of the sphere.
When the opening portion has a larger diameter than the sphere, the sphere can be
removed with an external force. The external force includes physical forces such
as a pressure caused by blowing with air or an inert gas, a pressure caused by
blowing a wash liquid, a magnetic suction force, an electrostatic force and a
centrifugal force. Unlike the field emission device of Example 17, in the field
emission device of Example 19 or 20, it is not required to dissipate the portion of
the electrically conductive material layer for a cathode electrode which covers the
sphere, or, in some cases, it is not required to dissipate the above portion, and
portions of the insulating layer and the gate-electrode-constituting layer, so that
there is an advantage that no residue arises from the electrically conductive
material layer for a cathode electrode, the insulating layer or the gate-electrode-constituting
layer.
-
In the field emission device of Example 19 or 20 to be described
later, preferably. at least the surface of the sphere used therefor is composed of a
material having a larger interfacial tension (surface tension) than material
constituting the electrically conductive material layer for a cathode electrode, or in
some cases, than materials constituting the above electrically conductive material
layer, the insulating layer and the gate-electrode-constituting layer. In the field
emission device of Example 20, the electrically conductive material layer for a
cathode electrode, the insulating layer and the gate-electrode-constituting layer
thereby do not cover at least top portions of the spheres. and there can be obtained
a state where the opening portion is formed in the insulating layer and the gate-electrode-constituting
layer from the beginning. The diameter of the opening
portion differs depending, for example, upon a relationship between the thickness
of a material for each of the electrically conductive material layer for a cathode
electrode, the insulating layer and the gate-electrode-constituting layer and the
diameter of each sphere; methods of forming the electrically conductive material
layer for a cathode electrode, the insulating layer and the gate-electrode-constituting
layer; and the interfacial tension (surface tension) of a material for
each of the electrically conductive material layer for a cathode electrode, the
insulating layer and the gate-electrode-constituting layer.
-
In the field emission device of Examples 19 or 20 to be described
later. it is sufficient that the spheres have the surfaces which satisfy the above
condition concerning the interfacial tension. That is, the portion having a larger
interfacial tension than any one of the electrically conductive material layer for a
cathode electrode, the insulating layer and the gate-electrode-constituting layer
may be only a surface of the sphere or may be the entirety of the sphere. The
material for the surface and/or the entirety of the sphere may be an inorganic
material, an organic material or a combination of an inorganic material with an
organic material. In the field emission device of Example 19 or 20, when the
electrically conductive material layer for a cathode electrode is composed of a
general metal material and when the insulating layer is composed of a silicon
oxide material such as glass, generally, a highly hydrophilic state is formed since
hydroxyl groups derived from adsorbed water are present on the metal material
and since dangling bonds of Si-O bonds and hydroxyl group derived from
adsorbed water are present on the surface of the insulating layer. It is therefore
particularly effective to spheres having hydrophobic surface-treatment layers.
The material for the hydrophobic surface-treatment layer includes fluorine resins
such as polytetrafluoroethylene. When the sphere has a hydrophobic surface-treatment
layer, and, if a portion inside the hydrophobic surface-treatment layer is
considered a core, the material for the core may be glass, ceramic or a polymer
material other than the fluorine resin.
-
Although not specially limited, the organic material for the sphere
is preferably a general-purpose polymer material. When the polymer material has
an extremely high polymerization degree or has an extremely large content of
double and triple bonds, too high a combustion temperature is required, and when
the spheres are removed by combustion, a detrimental effect may be caused on the
electrically conductive material layer for a cathode electrode, the insulating layer
and the gate-electrode-constituting layer. It is therefore preferred to select a
polymer material which is combustible or carbonizable at a temperature at which
no detrimental effect is caused on the above layers. When the insulating layer is
composed of a material which requires combustion at a post step, such as a glass
paste, it is preferred to select a polymer material which is combustible or
carbonizable at a calcining or sintering temperature of the glass paste, in order to
decrease the number of the manufacturing steps. Since a glass paste has a typical
calcining temperature of approximately 530 °C, the combustion temperature of
the polymer material is preferably approximately 350 to 500 °C. Typical
examples of the polymer material include styrene, urethane, acryl, vinyl,
divinylbenzene, melamine, formaldehyde and polymethylene homopolymers or
copolymers. For securing a reliable layout on the supporting substrate, there may
be used fixable spheres capable of adhering. As fixable spheres, spheres
composed of an acryl resin are used.
-
Otherwise, thermally expandable microspheres having a vinylidene
chloride-acrylonitrile copolymer as outer shells and encapsulating isobutane as a
foaming agent can be used as spheres. In the field emission device of Example
17, for example, the above thermally expandable microspheres are employed and
heated. In this case, a polymer constituting the outer shells is softened, and the
encapsulated isobutane is gasified to undergo expansion. As a result, there are
formed hollow true spheres having a diameter approximately 4 times as large as a
diameter found before the expansion. As a result, in the field emission device of
Example 17, the projection portions for emitting electrons and the concave
portions each of which is surrounded by the projection portion and reflects part of
form of the sphere can be formed in the electrically conductive material layer for a
cathode electrode. In addition to the above concave portions and the above
projection portions, further, the opening portions can be also formed in the gate-electrode-constituting
layer and the insulating layer. In the present specification,
the expansion of thermally expandable microspheres is also included in the
concept of the removal of the sphere. Then, thermally expandable microspheres
can be removed with a proper solvent.
-
In the field emission device of Example 17, the electrically
conductive material layer for a cathode electrode which layer covers the spheres
can be formed after a plurality of the spheres are arranged on the supporting
substrate. In this case or in the field emission device of Example 19 or 20 to be
described later, the method of arranging a plurality of the spheres includes a dry
method in which the spheres are sprayed onto the supporting substrate. For
spraying the spheres, there can be applied a method in which spacers are sprayed
for maintaining a panel distance at a constant distance in the field of producing
liquid crystal display devices. Specifically, a so-called spray gun for ejecting the
spheres through a nozzle with a compressed gas can be used. When the spheres
are ejected through the nozzle, the spheres may be in a state in which they are
dispersed in a volatile solvent. Otherwise, the spheres can be sprayed by means of
an apparatus or a method which is generally used in the field of an electrostatic
powder application or coating. For example, the spheres negatively charged can
be sprayed to the supporting substrate grounded, with an electrostatic spray gun,
using a corona discharge. Since the spheres used are very small as will be
described later, the spheres sprayed onto the supporting substrate adhere to the
surface of the supporting substrate, for example, with an electrostatic force, and
the adhering spheres do not easily fall off from the supporting substrate. When
the spheres are pressed after a plurality of the spheres are arranged on the
supporting substrate, overlapping of a plurality of the spheres on the supporting
substrate can be overcome, and the spheres can be densely arranged on the
supporting substrate so as to form a single layer so as to arrange one sphere and
another sphere side by side.
-
Otherwise, there may be employed a constitution in which, like the
field emission device of Example 18 to be described later, a composition layer
composed of a dispersion of the spheres and a cathode electrode material in a
dispersing agent is formed on the supporting substrate, thereby to arrange a
plurality of the spheres on the supporting substrate and to cover each sphere with
the cathode electrode composed of the cathode electrode material, and thereafter,
the dispersing agent is removed. The composition can have the property of a
slurry or paste, and the component and viscosity of the slurry or paste can be
selected as required depending upon the above properties be desired. Typically,
the cathode electrode material is preferably formed of fine particles having a
lower precipitation rate than the sphere in the dispersing agent. The material for
the above fine particles includes carbon, barium, strontium and iron. After the
dispersing agent is removed, the cathode electrode is calcined or sintered as
required. The method of forming the composition layer on the supporting
substrate includes a spraying method, a dropping method, a spin coating method
and a screen-printing method. When the spheres are arranged, each sphere is
concurrently covered (coated) with the electrically conductive material layer for a
cathode electrode, which material is the cathode electrode material. In some
method of forming the above composition layer, it is required to pattern the
electrically conductive material layer for a cathode electrode.
-
In the field emission device of Example 19 or 20 to be described
later, there may be employed a constitution in which a composition layer
composed of a dispersion of the spheres in a dispersing agent is formed on the
supporting substrate, thereby to arrange a plurality of the spheres on the
supporting substrate, and then the dispersing agent is removed. The composition
can have the property of a slurry or paste, and the component and viscosity of the
slurry or paste can be selected as required depending upon the above properties to
be desired. Typically, an organic solvent such as isopropyl alcohol is used as a
dispersing agent, and the dispersing agent can be removed by volatilization. The
method of forming the composition layer on the supporting substrate includes a
spraying method, a dropping method, a spin coating method and a screen-printing
method.
-
The gate-electrode-constituting layer and the electrically
conductive material layer for a cathode electrode extend in directions different
from each other (for example, a projection image of the gate-electrode-constituting
layer in the form of a stripe and the electrically conductive material
layer for a cathode electrode in the form of a stripe make an angle of 90°), and for
example, they are patterned in the form of stripes. Electrons are emitted from the
projection portions positioned in the electron-emitting region. It is therefore
functionally sufficient that the projection portions are present in the electron-emitting
region alone. Even if the projection portions and the concave portions
exist in a region different from the electron-emitting region, however, such
projection portions and concave portions remain covered with the insulating layer
and do not work to emit electrons. It is therefore no problem if the spheres are
arranged in the entire surface.
-
In contrast, when portions of the electrically conductive material
layer for a cathode electrode, the insulating layer and the gate-electrode-constituting
layer which portions cover the sphere are removed, arrangement
positions of individual spheres and formation positions of the opening portions
have one-to-one correspondence, so that the opening portions are formed in a
region different from the electron-emitting region. The opening portion formed in
a region different from the electron-emitting region will be referred to as
"ineffective opening portion" and distinguished from the original opening portion
which works for electron emission. Meanwhile, even if ineffective opening
portions are formed in a region other than the electron-emitting region, the
ineffective opening portions do not at all work as field emission devices, nor do
they cause any detrimental effect on the performance of the field emission devices
formed in the electron-emitting region. The reason therefor is as follows. Even if
the projection portion and the concave portion are exposed in the bottom portion
of the ineffective opening portion, no gate electrode is formed on the upper end
portion of the ineffective opening portion. Otherwise, even if the gate electrode is
formed in the upper end portion of the ineffective opening portion, neither the
projection portion nor the concave portion is exposed in the bottom portion; or
neither the projection portion nor the concave portion is exposed in the bottom
portion of the ineffective opening portion and no gate electrode is formed in the
upper end portion and the surface of the supporting substrate is merely exposed.
It is therefore no problem even if the spheres are arranged in the entire surface. A
hole formed in a boundary between the electron-emitting region and other region
is included in the opening portion.
-
The diameter of the sphere can be selected depending upon the
diameter of a desired opening portion, the diameter of the concave portion,
display screen dimensions of a flat-panel display constituted using the field
emission devices, the number of pixels, dimensions of the electron-emitting
region (overlapped region) and the number of the field emission devices per pixel.
The diameter of the sphere is preferably in the range of from 0.1 to 10 µm. For
example, spheres commercially available as spacers for liquid crystal display
devices are preferred since they have a particle diameter distribution of 1 to 3 %.
While the form of the sphere is ideally truly spherical, it is not necessarily
required to be truly spherical. In some method of producing the field emission
devices, opening portions or ineffective opening portions can be formed in
portions where the spheres are arranged, and it is preferred to arrange the spheres
in a density of approximately 100 to 5000 spheres/mm2. For example, when the
spheres are arranged in the supporting substrate in a density of approximately
1000 spheres/mm2, and for example, if the electron-emitting region has
dimensions of 0.5 mm x 0.2 mm, approximately 100 spheres are present in the
electron-emitting region, and approximately 100 projection portions are formed.
When the projection portions approximately in such a number are formed per
electron-emitting region, the fluctuation of diameters of the concave portions,
caused by the fluctuation in the particle diameter distribution and the sphericity of
the spheres, is nearly averaged, and the current density of emitted electrons per
pixel (or per subpixel) and the brightness come to be uniform.
-
In the field emission device of Example 17 or any one of Examples
18 to 20, part of the form of the sphere is reflected in the form of concave portion
constituting the electron-emitting portion. The profile of top end portion of each
projection portion may have an irregular convexo-concave form or may be flat. In
the field emission device of Example 17 or 18, in particular, the above top end
portion is formed by fracture or burst of the electrically conductive material layer
for a cathode electrode, so that the top end portion of each projection portion is
liable to have an irregular form. When the top end portion is sharpened by
fracture or burst, advantageously, the top end portion can function as a highly
efficient electron-emitting portion. In the field emission device of any one of
Examples 17 to 20, the projection portion surrounding the concave portion comes
to be ringed or circular, and in this case. the concave portion and the projection
portion as a whole have the form of crater or caldera.
-
The layout of the projection portions on the supporting substrate
may be regular or at random, and depends upon the method of arranging the
spheres. When the above dry method or a wet method is employed, the layout of
the projection portions on the supporting substrate comes to be at random.
In the field emission device of any one of Examples 17 to 20, when
the opening portion is formed in the insulating layer after the formation of the
insulating layer, there may be employed a constitution in which a protective layer
is formed for avoiding damage of top end portions of the projection portions after
the formation of the projection portions, and the protective layer is removed after
the opening portion is formed. The material for the protective layer includes
chromium.
-
The method of producing the field emission device of Example 17
will be explained with reference to Figs. 34A, 34B, 35A, 35B, 36A, 36B, 37A and
37B. Fig. 34A, Fig. 35A and Fig. 36A are schematic partial end views, Figs. 37A
and 37B are schematic partial cross-sectional views, and Fig. 34B, 35B and 36B
are schematic partial perspective views showing wider ranges than those in Figs.
34A, 35A and 36A.
[Step-1700]
-
First, a cathode electrode 411 covering a plurality of spheres 80 is
formed on the supporting substrate 10. Specifically, the spheres 80 are arranged
on the entire surface of the supporting substrate 10 made, for example, of glass.
The spheres 80 are composed, for example, of a polymethylene-based polymer
material, and they have an average particle diameter of approximately 5 µm and a
particle diameter distribution of less than 1 %. The spheres 80 are arranged on the
supporting substrate 10 at random at a density of approximately 1000
spheres/mm2 with a spray gun. The method of spraying the spheres with a spray
gun includes a method of spraying a mixture of the sphere with a volatile solvent
and a method of ejecting the spheres in a powder state from a nozzle. The
arranged spheres 80 are held on the supporting substrate 10 by an electrostatic
force. Figs. 34A and 34B shows such a state.
[Step-1710]
-
An electrically conductive material layer 411' for a cathode
electrode is formed on the spheres 80 and the supporting substrate 10. Figs. 35A
and 35B show a state where the electrically conductive material layer 411' for a
cathode electrode is formed. The electrically conductive material layer 411' for a
cathode electrode can be formed, for example, by screen-printing a carbon paste
in the form of a stripe. In this case, the spheres 80 are arranged on the entire
surface of the supporting substrate 10, so that some of the spheres 80 are naturally
not covered with the electrically conductive material layer 411' as shown in Fig.
35B. Then, the electrically conductive material layer 411' is dried, for example, at
150 °C for removing water and a solvent contained in the electrically conductive
material layer 411' and flattening the electrically conductive material layer 411'.
At this temperature, the spheres 80 undergo any state change and/or chemical
change. The above screen-printing using a carbon paste may be replaced with a
method in which the electrically conductive material layer 411' for a cathode
electrode is formed on the entire surface and the electrically conductive material
layer 411' is patterned by general lithography and a general dry etching method to
form the electrically conductive material layer 411' for a cathode electrode in the
form of a stripe. When the lithography is applied, generally, a resist layer is
formed by a spin coating method. In the spinning, if the number of spinning of
the supporting substrate 10 is 500 rpm and if the spinning time period is
approximately several seconds long, the spheres 80 are held on the supporting
substrate 10 without dropping off or shifting in position.
[Step-1720]
-
Portions of the electrically conductive material layer 411' for a
cathode electrode which portions cover the spheres 80 are removed by removing
the spheres 80. whereby there is formed a cathode electrode 41 having projection
portions 411A and concave portions 411B each of which is surrounded by the
projection portion 411A and reflects part of form of each sphere 80. Figs. 36A
and 36B shows the thus-obtained state. Specifically, the spheres 80 are
combusted by heating around 530 °C while the electrically conductive material
layer 411' for a cathode electrode is also calcined or sintered. The pressure in
each closed space near each sphere 80 increases together with the combustion of
the sphere 80, and a portion of the electrically conductive material layer 411'
which portion covers the sphere 80 bursts when a certain pressure durability limit
is exceeded, and such a portion is removed. As a result, the projection portions
411A and the concave portions 411B are formed in part of the cathode electrode
411 formed on the supporting substrate 10. When some portions of the sphere
remain as a residue after the removal of the spheres, the residue can be removed
with a proper wash liquid depending upon a material constituting the spheres
used.
[Step-1730]
-
Then, the insulating layer 12 is formed on the cathode electrode
411 and the supporting substrate 10. Specifically, for example, a glass paste is
screen-printed on the entire surface to form a layer having a thickness of
approximately 5 µm. Then, the insulating layer 12 is dried, for example, at 150
°C to remove water and a solvent contained the insulating layer 12 and to flatten
the insulating layer 12. The above screen-printing using a glass paste may be
replaced, for example, with the formation of an SiO2 layer by a plasma CVD
method.
[Step-1740]
-
Then, the gate electrode 313 in the form of a stripe is formed on the
insulating layer 12 (see Fig. 37A). The extending direction of a projection image
of the gate-electrode-constituting layer in the form of a stripe makes an angle of
90° with the extending direction of a projection image of the electrically
conductive material layer for a cathode electrode in the form of a stripe.
[Step-1750]
-
Then, in the electron-emitting region where the projection image of
the gate electrode 313 and the projection image of the cathode electrode 411
overlap, the opening portion 14 are formed through the gate electrode 313 and the
insulating layer 12, thereby to expose a plurality of the projection portions 41lA
and the concave portions 411B in the bottom portion of the opening portion 14.
The opening portion 14 can be obtained by forming a resist mask according to
general lithography and etching through the resist mask. Preferably, the etching is
carried out under a condition sufficiently high etching selectivity to the cathode
electrode 411 is secured. Otherwise, after the formation of the projection portions
411A, preferably, a protective layer composed of chromium is formed in advance,
and after the opening portion 14 is formed, the protective layer is removed. Then,
the resist mask is removed. In this manner, the field emission device shown in
Fig. 37B can be obtained.
-
As a variant of the method of producing the field emission device
of Example 17, there may be employed a constitution in which [Step-1730] to
[Step-1750] are carried out after [Step-1710] and then [Step-1720] is carried out.
In this case, the combustion of the spheres and the calcining or sintering of the
material for an insulating layer 12 can be carried out concurrently.
-
Otherwise, [Step-1730] is carried out after [Step-1710], and in a
step similar to [Step-1740], further, a gate-electrode-constituting layer free of the
opening portion in the form of a stripe is formed on the insulating layer. Then,
[Step-1720] is carried out. In this manner, portions of the electrically conductive
material layer 411' for a cathode electrode . the insulating layer 12 and the gate-electrode-constituting
layer which portions cover the spheres 80 are removed,
whereby the opening portion can be formed in the gate electrode 313 and the
insulating layer 12 and the electron-emitting portion having the projection portion
411A and the concave portion 411 B which is surrounded by the projection portion
411A and reflects part of the form of each sphere 80 can be formed in the cathode
electrode 411 which is positioned in the bottom portion of the opening portion.
That is, the pressure in each closed space near each sphere 80 increases together
with the combustion of the sphere 80, and portions of the electrically conductive
material layer 411' for a cathode electrode, the insulating layer 12 and the gate-electrode-constituting
layer which portions cover the sphere are burst when a
certain pressure durability limit is exceeded, and the opening portion is formed
together with the projection portion 411A and the concave portion 411B. Further,
the sphere 80 is removed. The opening portion is formed in the gate electrode 313
and the insulating layer 12 and reflects part of the sphere 80. In the bottom
portion of the opening portion, there remains the projection portion 411A for
emitting electrons and the concave portion 411B which is surrounded by the
projection portion 411A and reflects part of the form of the sphere.
Example 18
-
Example 18 is a variant of Example 17. The method of producing
a crater-type field emission device of Example 18 will be explained with reference
to Figs. 38A, 38B and 38C. The method of Example 18 differs from the method
of Example 17 in that the step of arranging a plurality of the spheres 80 on the
supporting substrate 10 includes the steps of forming a composition layer 81
composed of a composition which is a dispersion of the spheres 80 and the
cathode electrode material in a dispersing agent on the supporting substrate 10,
thereby to arrange a plurality of the spheres on the supporting substrate 10,
covering the spheres 80 with the cathode electrode 411 composed of the cathode
electrode material, and then, removing the dispersing agent, that is, the above step
is a wet method.
[Step-1800]
-
First, a plurality of the spheres are arranged on the supporting
substrate 10. Specifically, the composition layer 81 composed of a composition
which is a dispersion of the spheres 80 and the cathode electrode material 81B in
a dispersing agent layer 81A is formed on the supporting substrate 10. That is, for
example, isopropyl alcohol is used as a dispersing agent, and a composition is
prepared by dispersing the spheres 80 which are composed of a polymethylene
polymer material and have an average particle diameter of approximately 5 µm
and carbon particles having an average particle diameter of 0.05 µm as the
cathode electrode material 81B in the dispersing agent 81A. The composition is
screen-printed on the supporting substrate 10 in the form of a stripe, to form the
composition layer 81. Fig. 38A shows a state found immediately after the
formation of the composition layer 81.
[Step-1810]
-
In the composition layer 81 held on the supporting substrate 10, the
spheres 80 precipitates soon to be arranged on the supporting substrate 10 and the
cathode electrode material 81B also precipitates to form an electrically conductive
material layer 411' (composed of the cathode electrode material 81B) for a
cathode electrode, whereby a plurality of the spheres 80 can be arranged on the
supporting substrate 10 and the spheres 80 can be covered with the electrically
conductive material layer 411' (composed of the cathode electrode material 81B)
for a cathode electrode. Fig. 38B shows the thus-obtained state.
[Step-1820]
-
Then, the dispersing agent 81A is removed by volatilization. Fig.
38C shows the thus-obtained state.
[Step-1830]
-
Then, steps similar to [Step-1720] to [Step-1750] in Example 17 or
variants of the method of producing the field emission device of Example 17 is
carried out, whereby an field emission device similar to the device shown in Fig.
37B can be completed.
Example 19
-
Example 19 is also a variant of Example 17. In the method of
producing a crater-type field emission device in Example 19, more specifically,
the step of forming the cathode electrode in the form of a stripe on the supporting
substrate comprises the steps of arranging a plurality of the spheres on the
supporting substrate; forming a cathode electrode which has a plurality of the
projection portions for emitting electrons and the concave portions each of which
is surrounded by the projection portion and reflects part of the sphere, on the
supporting substrate; and removing the spheres. The spheres are arranged on the
supporting substrate by spraying. The spheres have a hydrophobic surface-treatment
layer. The method of producing such an field emission device will be
explained with reference to Figs. 39A, 39B and 39C hereinafter.
[Step-1900]
-
First, spheres 180 are arranged on the supporting substrate 10.
-
Specifically, a plurality of the spheres 180 are arranged on the supporting
substrate 10 made, for example, of glass. The spheres 180 are formed by
providing a core material 180A composed, for example, of a divinylbenzene
polymer material and coating the core material 180A with a surface-treatment
layer 180B composed of a polytetrafluoroethylene resin, and the spheres 180 have
an average diameter of approximately 5 µm and a particle diameter distribution of
less than 1 %. The spheres 180 are arranged on the supporting substrate 10 in a
density of approximately 1000 spheres/mm2 at random with a spray gun. The
arranged spheres 180 are held on the supporting substrate 10 by an electrostatic
force. Fig. 39A shows the thus-obtained state.
[Step-1910]
-
Then, on the supporting substrate 10 is formed a cathode electrode
411 (constituted of an electrically conductive material layer for a cathode
electrode) having projection portions 411A and concave portion 411B each of
which is surrounded by the projection portion 411A and reflects part of form of
the sphere 180, the projection portions 411A being formed around the spheres
180. Specifically, as described with regard to the field emission device in
Example 17, for example, a paste is screen-printed in the form of a stripe. In the
field emission device in Example 19, the surface of each sphere 180 has
hydrophobic nature due to the surface-treatment layer 180B, so that the paste
screen-printed on the sphere 180 is immediately repelled and dropped off and is
deposited around the sphere 180 to form the projection portion 411 A. The top
end of each projection portion 411A is not so sharpened as that in the field
emission device in Example 17. A portion of the electrically conductive material
layer for a cathode electrode which portion enters between the sphere 180 and the
supporting substrate 10 constitutes the concave portion 411B. While Fig. 39B
shows a state where a gap is present between the cathode electrode 411 and the
sphere 180, the cathode electrode 411 and the sphere 180 are in contact with each
other in some cases. Then, the cathode electrode 411 is dried, for example, at 150
(C. Fig. 39B shows the thus-obtained state.
-
Then, an external force is exerted on the spheres 180 to remove the spheres
180 from the supporting substrate 10. Specifically, the method of removal
includes a washing method and a method of blowing a compressed gas. Fig. 39C
shows the thus-obtained state. The spheres can be also removed by the state
change/chemical change of the spheres, more specifically, for example, by
combustion, which is also applicable to the field emission device in Example 20
to be described below.
[Step-1930]
-
Then, [Step-1730] to [Step-1750] for the field emission device in
Example 17 are carried out, whereby there can be obtained an field emission
device which is almost the same as the device shown in Fig. 37B.
-
In a variant of the method of producing the field emission device in
Example 19, there may be employed a constitution in which [Step-1730] to [Step-1750]
for the field emission device in Example 17 are carried out after [Step-1910]
and then [Step-1920] is carried out.
Example 20
-
In the method of producing a crater-type field emission device in
Example 20, more specifically, the step of forming the cathode electrode in the
form of a stripe on the supporting substrate comprises the steps of arranging a
plurality of the spheres on the supporting substrate; and forming a cathode
electrode which has a plurality of the projection portions for emitting electrons
and the concave portions each of which is surrounded by the projection portion
and reflects part of the sphere, on the supporting substrate, each projection portion
being formed in a circumference of each sphere. When an insulating layer is
formed on the entire surface, the insulating layer having opening portions above
the spheres is formed on the cathode electrode and the supporting substrate. The
spheres are removed after the opening portions are formed. In the method of
producing the field emission device in Example 20, a plurality of the spheres are
arranged on the supporting substrate by spraying the spheres. Each sphere has a
hydrophobic surface-treatment layer. The method of producing the field emission
device in Example 20 will be explained with reference to Figs. 40A, 40B, 41A
and 41B.
[Step-2000]
-
First, a plurality of the spheres 180 are arranged on the supporting
substrate 10. Specifically, a step similar to the [Step-1900] in Example 19 is
carried out.
[Step-2010]
-
Then, formed on the supporting substrate 10 is a cathode electrode
411 having a plurality of projection portions 41lA for emitting electrons and
concave portions each of which is surrounded by the projection portion 411A and
reflects part of the form of the sphere 180, each projection portion 411A being
formed in a circumference of each sphere 180. Specifically, a step similar to
[Step-1910] in Example 19 is carried out.
[Step-2020]
-
An insulating layer 12 having opening portions 14A above the
spheres is formed on the cathode electrode 411 and the supporting substrate 10.
Specifically, a glass paste is screen-printed on the entire surface to form a layer
having a thickness of approximately 5 µm. The screen-printing of a glass paste
can be carried out in the same manner as in the field emission device of Example
17. The surface of each sphere 180 has hydrophobic nature due to the surface-treatment
layer 180B, so that the screen-printed glass paste is immediately
repelled and dropped off and that a portion of the insulating layer 12 which
portion is on each sphere 180 shrinks due to its surface tension. As a result, the
top portion of each sphere 180 is exposed into the opening portion 14A without
being covered with the insulating layer 12. Fig. 40A shows the thus-obtained
state. In a shown embodiment, the top end portion of the opening portion 14A has
a larger diameter than the sphere 180. When the surface-treatment layer 180B has
a smaller interfacial tension (surface tension) than the glass paste, the opening
portion 14A tends to have a smaller diameter. When the surface-treatment layer
180B has an extremely larger interfacial tension than the glass paste, the opening
portion 14A tends to have a larger diameter. Then, the insulating layer 12 is
dried, for example, at 150 °C.
[Step-2050]
-
Then, a gate electrode 313 having an opening portion 14B
communicating with the opening portion 14A is formed on the insulating layer 12.
Specifically, a paste is screen-printed in the form of a stripe. The screen-printing
of a paste can be carried out in the same manner as in the field emission device of
Example 17. Since, however, the surface of the sphere 180 has higher
hydrophobic nature due to the surface-treatment layer 180B, the paste screen-printed
on the sphere 180 is immediately repelled and shrinks due to its own
surface tension to form a state where it adheres only to the surface of the
insulating layer 12. In this case, the gate electrode 313 may be formed so as to
droop from the opening end portion of the insulating layer 12 into the opening
portion 14A to some extent. Then, the gate electrode 313 is dried, for example, at
150 °C. Fig. 40B shows the thus-completed state. When the surface-treatment
layer 180B has a smaller interfacial tension than the paste, the opening portion
14A tends to have a smaller diameter. When the surface-treatment layer 180B has
an extremely larger interfacial tension than the paste, the opening portion 14A
tends to have a larger diameter.
[Step-2040]
-
Then, the sphere 180 exposed in the opening portion 14A and 14B
is removed. Specifically, the sphere 18 is combusted by heating the sphere at
approximately 530 °C. a typical temperature for calcining or sintering a glass
paste, which heating also works to calcine or sinter the cathode electrode 411 and
the insulating layer 12. In this case, the insulating layer 12 and the gate electrode
313 have the opening portions 14A and 14B from the beginning unlike the field
emission device in Example 17, so that part of the cathode electrode 411, the
insulating layer 12 or the gate electrode 313 is not dissipated in any case, and the
sphere 180 is readily removed. When the upper end portion of the opening
portions 14A and 14B has a larger diameter than the sphere 180, the sphere can be
removed by an external force such as washing or blowing of a compressed gas
without combusting the sphere 180. Fig. 41A shows the thus-completed state.
[Step-2050]
-
Part of the insulating layer 12 which part corresponds to the side
wall surface of the opening portion 14 is isotropically etched, whereby an field
emission device shown in Fig. 41B can be completed. In this embodiment, the
lower end of the gate electrode 313 faces downward, which is preferred for
increasing the electric field intensity in the opening portion 14.
Example 21
-
Fig. 42A shows a schematic partial cross-sectional view of an
edge-type field emission device. The edge-type field emission device has a
cathode electrode (electron-emitting layer) 111 formed on the supporting substrate
10 in the form of a stripe; an insulating layer 12 formed on the supporting
substrate 10 and the cathode electrode 111; and a gate electrode 313 formed on
the insulating layer 12 in the form of a stripe. An opening portion 14 is formed
through the gate electrode 313 and the insulating layer 12. An edge portion 111A
of the cathode electrode 111 is exposed in the bottom portion of the opening
portion 14. A voltage is applied to the cathode electrode 111 and the gate
electrode 313, whereby electrons are emitted from the edge portion 111A of the
cathode electrode 111.
-
As shown in Fig. 42B, a concave portion 10A may be formed in the
supporting substrate 10 below the cathode electrode 111 inside the opening
portion 14. Otherwise, as Fig. 42C shows a schematic partial cross-sectional
view, the edge-type field emission device may have a first gate electrode 13A
formed on the supporting substrate 10; a lower insulating layer 12A formed on the
supporting substrate 10 and the first gate electrode 13A; a cathode electrode 111
formed on the lower insulating layer 12A; an upper insulating layer 12B formed
on the lower insulating layer 12A and the cathode electrode 111; and a second
gate electrode 313B formed on the upper insulating layer 12B. And, an opening
portion 14 is formed through the second gate electrode 313B, the upper insulating
layer 12B, the cathode electrode 111 and the lower insulating layer 12A. An edge
portion 111A of the cathode electrode 111 is exposed on a side wall surface of the
opening portion 14. A voltage is applied to the cathode electrode 111 and the first
and second gate electrodes 13A and 313B, whereby electrons are emitted from the
edge portion 111A of the cathode electrode 111 which edge portion corresponds
to an electron-emitting portion.
-
The method of producing the edge-type field emission device
shown, for example, in Fig. 42C will be explained with reference to Figs. 43A,
43B and 43C showing schematic partial end views of the supporting substrate and
the like.
[Step-2100]
-
First, an approximately 0.2 µm thick tungsten layer is formed on
the supporting substrate 10 made, for example, of a glass by a sputtering method,
and the tungsten layer is patterned by photolithography and a dry etching method,
to form the first gate electrode 13A in the from of a stripe. Then, the lower
insulating layer 12A, which is composed of SiO2 and has a thickness of
approximately 0.3 µm, is formed on the entire surface, and then the cathode
electrode 111 constituted of an electrically conductive material layer composed of
tungsten in the form of a stripe is formed on the lower insulating layer 12A (see
Fig. 43A).
[Step-2110]
-
Then, the upper insulating layer 12B, which, for example, is
composed of SiO2 and has a thickness of 0.7 µm. is formed on the entire surface,
and then the second gate electrode 313B in the form of a stripe is formed on the
upper insulating layer 12B (see Fig. 43B). The second gate electrode 313B is
composed of a gas-trapping material.
[Step-2120]
-
Then, a resist layer 90 is formed on the entire surface, and a resist
opening portion 90A is formed in the resist layer 90 such that part of the surface
of the second gate electrode 313B is exposed. The resist opening portion 90A has
a rectangular form when viewed as a plan view. The rectangular form has a major
side length of 100 µm and a minor side length of several to 10 µm. Then, the
second gate electrode 313B exposed in the bottom portion of the resist opening
portion 90A is anisotropically etched, for example, by an RIE method, to form an
opening portion. Then, the upper insulating layer 12B exposed in the bottom
portion of the opening portion is isotropically etched to form an opening portion
(see Fig. 43C). Since the upper insulating layer 12B is composed of SiO2, wet
etching is carried out using a buffered hydrofluoric acid aqueous solution. The
side wall surface of the opening portion in the upper insulating layer 12B recedes
from the opening end portion of the opening portion formed in the second gate
electrode 313B. In this case, the recess amount can be controlled by adjusting the
etching time period. In this embodiment, the wet etching is carried out until the
lower end of the opening portion formed in the upper insulating layer 12B recedes
from the opening end portion of the opening portion formed in the second gate
electrode 313B.
-
The cathode electrode 111 exposed in the bottom portion of the
opening portion is dry-etched under a condition where ions are used as main
etching species. In the dry-etching using ions as main etching species, ions as
charged particles can be accelerated by applying a biased voltage to an object to
be etched or utilizing interaction of plasma and an electric field, and generally,
anisotropic etching proceeds, so that the etched object has a perpendicular wall as
a processed surface. In this step, however, the main etching species contain
incidence components having angles different from the perpendicularity, and
obliquely entering components are also generated due to scattering on the end
portion of the opening portion, so that, at some probability, main etching species
enter regions which ion originally should not reach since the regions are shielded
by the opening portion. In this case, main etching species having a smaller
incidence angle with regard to the normal of the supporting substrate 10 show a
higher entering probability, and main etching species having a larger incidence
angle show a lower entering probability.
-
Therefore, while the position of upper end portion of the opening
portion formed in the cathode electrode 111 is nearly lined up with the lower end
portion of the opening portion formed in the upper insulating layer 12B, the
position of the lower end portion of the opening portion formed in the cathode
electrode 111 is projected from the upper end portion thereof. That is, the
thickness of the edge portion 111A of the cathode electrode 111 decreases toward
the leading end portion in the projection direction, and the edge portion 111A is
sharpened. For example, when SF6 is used as an etching gas, the cathode
electrode 111 can be excellently processed.
-
The lower insulating layer 12A exposed in a bottom portion of the
opening portion formed in the cathode electrode 111 is isotropically etched, to
form an opening portion in the lower insulating layer 12A, whereby the opening
portion 14 is completed. In this embodiment, wet etching is carried out using a
buffered hydrofluoric acid aqueous solution. The side wall surface of the opening
portion formed in the lower insulating layer 12A recedes from the lower end
portion of the opening portion formed in the cathode electrode 111. In this case,
the recess amount can be controlled by adjusting the etching time period. After
the completion of the opening portion 14, the resist layer 90 is removed, whereby
the constitution shown in Fig. 42C can be obtained.
Example 22
-
Example 22 is concerned with the method of producing a Spindt-type
field emission device different from that in Example 2. The method of
producing such a Spindt-type field emission device will be explained hereinafter
with reference to Figs. 44A, 44B, 45A, 45B, 46A and 46B showing schematic
partial end views of a supporting substrate, etc. The Spindt-type field emission
device in this Example is produced basically according to the steps of;
- (a') forming a cathode electrode 511 on a supporting substrate 510,
- (b') forming an insulating layer 512 on the cathode electrode 511
and the supporting substrate 510,
- (c') forming a gate electrode 313 on the insulating layer 512,
- (d') forming an opening portion 514 having the cathode electrode
511 exposed in a bottom portion thereof, at least in the insulating layer 512,
- (e') forming an electrically conductive material layer 521 for an
electron-emitting portion on the entire surface including the inside of the opening
portion 514,
- (f') forming a mask material layer 522 on the electrically
conductive material layer 521 so as to mask a region of the electrically conductive
material layer 521 which region is positioned in a central portion of the opening
portion 514, and
- (g') etching the electrically conductive material layer 521 and the
mask material layer 522 under an anisotropic etching condition where an etching
rate of the electrically conductive material layer 521 in the direction perpendicular
to the supporting substrate 510 is higher than an etching rate of the mask material
layer 522 in the direction perpendicular to the supporting substrate 510, to form an
electron-emitting portion 15D which is constituted of the electrically conductive
material layer 521 and has a top end portion having a conical form, on the cathode
electrode 511 exposed in the opening portion 514.
-
[Step-2200]
-
The cathode electrode 511 composed of chromium (Cr) is formed
on the supporting substrate 510 prepared, for example, by forming an
approximately 0.6 µm thick SiO2 layer on a glass substrate. Specifically, an
electrically conductive material layer composed of chromium for a cathode
electrode is deposited on the supporting substrate 510, for example, by a
sputtering method or a CVD method, and the electrically conductive material
layer is patterned, whereby there can be formed the electrically conductive
material layer including a plurality of cathode electrodes 511 and being in the
form of a stripe extending in parallel in a row direction. The electrically
conductive material layer for a cathode electrode has a width, for example, of 50
(m and one electrically conductive material layer is spaced from another
electrically conductive material layer at a distance, for example, of 30 µm. Then,
the insulating layer 512 composed of SiO2 is formed on the entire surface,
specifically, on the cathode electrode 511 and the supporting substrate 510 by a
plasma CVD method using TEOS (tetraethoxysilane) as a source gas. The
insulating layer 512 has a thickness of approximately 1 µm. Then, the gate
electrode 313 is formed on the entire surface on the insulating layer 512, the gate
electrode 313 being formed of a gate-electrode-constituting layer in the form of a
stripe and extending in the direction at right angles with the electrically
conductive material layer for a cathode electrode.
-
Then, in an electron-emitting region where the electrically
conductive material layer for a cathode electrode and the gate-electrode-constituting
layer overlap, that is, in a one pixel region, opening portions 514 are
formed through the gate-electrode-constituting layer and the insulating layer 512.
The opening portion 514 has, for example, the form of a circle having a diameter
of 0.3 µm when viewed as a plan view. Generally, hundreds to thousands of
opening portions 514 are formed per one pixel region (one electron-emitting
region). For forming the opening portions 514, while a resist layer formed by
general photolithography is used as a mask, first, the opening portions 514 are
formed in the gate-electrode-constituting layer, and the opening portions 514 are
formed in the insulating layer 512. After RIE, the resist layer is removed by
ashing (see Fig. 44A).
[Step-2210]
-
Then, an adhesion layer 520 is formed on the entire surface by a
sputtering method (see Fig. 44B). The adhesion layer is provided for improving
the adhesion of an electrically conductive material layer 521 to be formed in a
step to follow to the insulating layer 512 exposed in a non-formed regions of the
gate-electrode-constituting layer and to the side wall surfaces of the opening
portions 514. On condition that tungsten is used to form the electrically
conductive material layer 521, the adhesion layer 520, which is composed of
tungsten, is formed as a 0.07 µm thick layer by a DC sputtering method.
[Step-2220]
-
The electrically conductive material layer 521 for an electron-emitting
portion is formed on the entire surface including the inside of the
opening portion 514 by a hydrogen reduction pressure reduced CVD method, the
electrically conductive material layer 521 having a thickness of approximately 0.6
µm and being composed of tungsten (see Fig. 45A). In the surface of the formed
electrically conductive material layer 521, formed is a recess 521A reflecting a
step between the top end surface and the surface of bottom portion of the opening
portion 514.
[Step-2230]
-
A mask material layer 522 is formed so as to cover a region
(specifically, the recess 521A) of the electrically conductive material layer 521
which region is positioned in the central portion of the opening portion 514.
Specifically, a 0.35 µm thick resist layer as the mask material layer 522 is formed
on the electrically conductive material layer 521 by a spin coating method (see
Fig. 45B). The mask material layer 522 absorbs the recess 521A of the
electrically conductive material layer 521 to form a nearly flat surface. Then, the
mask material layer 522 is etched by an RIE method using oxygen-containing gas.
The etching is terminated when a flat surface of the electrically conductive
material layer 521 is exposed, whereby the mask material layer 522 remains so as
to form a flat surface by filling itself in the recess 521A of the electrically
conductive material layer 521 (see Fig. 46A).
[Step-2240]
-
Then, the electrically
conductive material layer 521, the
mask
material layer 522 and the
adhesion layer 520 are etched to form a conical
electron-emitting
portion 15D (see fig. 46B). These are etched under an
anisotropic etching condition where an etching rate of the electrically
conductive
material 521 is higher than an etching rate of the
mask material layer 522. The
following Table 4 shows the etching condition.
Etching condition of electrically conductive material layer 521, etc. |
SF6 flow rate | 150 SCCM |
O2 flow rate | 30 SCCM |
Ar flow rate | 90 SCCM |
Pressure | 35 Pa |
RF power | 0.7 kW (13.56 MHz) |
[Step-2250]
-
Inside the opening portion 514 formed in the insulating layer 512,
the side wall surface of the opening portion 514 is receded under an isotropic
etching condition, whereby an field emission device shown in Fig. 47 is
completed. The isotropic etching can be carried out a dry etching method using
radical as main etching species such as chemical dry etching, or by a wet etching
method using an etching solution. As an etching solution, for example, there may
be used a mixture containing a 49 % hydrofluoric acid aqueous solution and pure
water in a 49 % hydrofluoric acid aqueous solution/pure water volume ratio of
1/100.
-
The mechanism of forming the field emission device 15D in [Step2240]
will be explained with reference to Figs. 48A and 48B. Fig. 48A
schematically shows how the surface profile of a material to be etched changes at
constant time intervals as the etching proceeds, and Fig. 48B is a graph showing a
relationship between an etching time and a thickness of the material being etched
in the center of the opening portion 514. The mask material layer has a thickness
hp in the center of the opening portion 514, and the electron-emitting portion 15D
has a height he in the center of the opening portion 514.
-
Under the etching condition shown in Table 4, the etching rate of
the electrically conductive material layer 521 is naturally higher than the etching
rate of the mask material layer 522 composed of a resist material. In a region
where no mask material layer 522 is present, the electrically conductive material
layer 521 immediately begins to be etched, and the surface of the material being
etched readily goes down. In contrast, in a region where the mask material layer
522 is present, the electrically conductive material layer 521 begins to be etched
only after the mask material layer 522 is removed first. While the mask material
layer 522 is etched, therefore, the decremental rate of thickness of the material
being etched is low (hp decremental interval), and the decremental rate of
thickness of the material being etched comes to be as high as the etching rate in
the region where no mask material layer 522 is present only when the mask
material layer 522 disappears (he decremental interval). The time at which the he
decremental interval begins comes the last in the center of the opening portion
where the mask material layer 522 has a largest thickness, and comes earlier in a
region nearer to the circumference of the opening portion 514 where the mask
material layer 522 has a smaller thickness. In the above manner, the electron-emitting
portion 15D having a conical form is formed.
-
The ratio of the etching rate of the electrically conductive material
layer 521 to the etching rate of the mask material layer 522 composed of a resist
material will be referred to as "selective ratio to a resist". The selective ratio to a
resist is an important factor for determining the height and the form of the
electron-emitting portion 15D. This point will be explained with reference to
Figs. 49A, 49B and 49C. Fig. 49A shows a form of the electron-emitting portion
15D when the selective ratio to a resist is relatively small. Fig. 49C shows a form
of the electron-emitting portion 15D when the selective ratio to a resist is
relatively large. Fig. 49B shows a form of the electron-emitting portion 15D
when the selective ratio to a resist is intermediate. It is seen that with an increase
in the selective ratio to a resist, the film decrease of the electrically conductive
material layer 521 is sharp as compared with the film decrease of the mask
material layer 522, so that the electron-emitting portion 15D has a larger height
and a sharper form. The selective ratio to a resist decreases with an increase in the
O2 flow rate relative to the SF6 flow rate. When an etching apparatus which
makes it possible to change the incidence energy of ion by co-using substrate bias
is used, the selective ratio to a resist can be decreased by increasing the RF bias
power or decreasing the frequency of AC current for bias application. When the
selective ratio to a resist is selected, it is at least 1.5, preferably at least 2, more
preferably at least 3.
-
In the above etching, naturally, it is required to secure a high
selective etching ratio to the gate electrode 313 and the cathode electrode 511.
Under the condition shown in Table 4, no problem is caused. The reason therefor
is as below. The material constituting the gate electrode 313 or the cathode
electrode 511 is hardly etched with fluorine-containing etching species so long as
a proper material is selected. Under the above condition, a selective etching ratio
of approximately 10 or more can be obtained.
Example 23
-
Example 23 is a variant of Example 22. In the production method
in Example 23, the region of the electrically conductive material which region is
covered with the mask material layer can be narrowed as compared with the
production method in Example 22. In the method of producing a Spindt-type field
emission device in Example 23, a nearly funnel-like recess having a columnar
portion and a widened portion communicating with the upper end of the columnar
portion is formed in a surface of the conductive material layer by utilizing a step
between the upper end surface and the surface of bottom portion of the opening
portion, and in the step (f'), the mask material layer is formed on the entire surface
of the electrically conductive material layer. Then, the mask material layer and
the electrically conductive material layer are removed in a plane in parallel with
the surface of the supporting substrate, whereby the mask material layer is
retained in the columnar portion.
-
The method of producing the Spindt-type field emission device in
Example 23 will be explained hereinafter with reference to Figs. 50A, 50B, 51A,
51B, 52A and 52B showing schematic partial end views of a supporting substrate,
etc.
[Step-2300]
-
First, the cathode electrode 511 is formed on the supporting
substrate 510. That is, an electrically conductive material layer for a cathode
electrode, including the cathode electrodes 511, is formed by stacking a TiN layer
(thickness 0.1 µm), a Ti layer (thickness 5 nm), an Al-Cu layer (thickness 0.4
µm), a Ti layer (thickness 5 nm), a TiN layer (thickness 0.02 µm) and a Ti layer
(thickness 0.02 µm) in this order, for example, by a DC sputtering method to form
a stacked layer and patterning the stacked layer in the form of a stripe. Figures
show the cathode electrode 511 as a single layer. Then, a 0.7 µm thick insulating
layer 512 is formed on the entire surface, specifically, on the supporting substrate
510 and the cathode electrode 511 by a plasma CVD method using TEOS
(tetraethoxysilane) as a source gas. Then, a gate-electrode-constituting layer in
the form of a stripe, including the gate electrodes 313, is formed on the insulating
layer 512.
-
Further, a 0.2 µm thick etching-stop layer 523 composed of SiO2 is
formed on the entire surface. The etching-stop layer 523 is not essential for the
function of the field emission device but works to protect the gate electrode 313
when the electrically conductive material layer 521 is etched in a step to come
later. When the gate electrode 313 has sufficiently high etching durability against
an etching condition for the electrically conductive material layer 521, the
etching-stop layer 523 may be omitted. Then, an opening portion 514 is formed
through the etching stop layer 523, the gate electrode 313 and the insulating layer
512 by an RIE method. The cathode electrode 511 is exposed in a bottom portion
of the opening portion 514. In this manner, a state shown in Fig. 50A is obtained.
[Step-2310]
-
Then, a 0.03 µm thick adhesion layer 520 composed, for example,
of tungsten is formed on the entire surface including the inside of the opening
portion 514 (see Fig. 50B). Then, an electrically conductive material layer 521
for an electron-emitting portion is formed on the entire surface including the
inside of the opening portion 514. In Example 23, the thickness of the electrically
conductive material layer 521 is determined such that a recess 521A having a
larger depth than the recess 521A in Example 22 is formed in the surface. That is,
the thickness of the electrically conductive material layer 521 is properly
determined, whereby there can be formed a nearly funnel-like recess 521A having
a columnar portion 521B and a widened portion 521C communicating with the
upper end of the columnar portion in the surface of the conductive material layer
521 by utilizing a step between the upper end surface and the surface of bottom
portion of the opening portion 514.
[Step-2320]
-
Then, an approximately 0.5 µm thick
mask material layer 522
composed of copper (Cu) is formed on the entire surface of the electrically
conductive material layer 521 by an electroless plating method (see Fig. 51A).
Table 5 shows a condition of the electroless plating.
Plating solution | Copper sulfate (CuSO4•5H2O) | 7 g/liter |
Formalin (37% HCHO) | 20 ml/liter |
Sodium hydroxide (NaOH) | 10 g/liter |
Potassium sodium tartarate | 20 g/liter |
Plating bath temperature | 50°C |
[Step-2330]
-
Then, the mask material layer 522 and the electrically conductive
material layer 521 are removed in a plane in parallel with the surface of the
supporting substrate 510, to retain the mask material layer 522 in the columnar
portion 521B (see Fig. 51B). The above removal can be carried out, for example
by a chemical/mechanical polishing (CMP) method.
[Step-2340]
-
Then, the electrically conductive material layer 521, the mask
material layer 522 and the adhesion layer 520 are etched under an anisotropic
condition where etching rates of the electrically conductive material layer 521 and
the adhesion layer 520 are higher than an etching rate of the mask material layer
522. As a result, an electron-emitting portion 15D having a conical form is
formed in the opening portion 514 (see Fig. 52A). When the top end portion of
the electron-emitting portion 15D has a residual mask material layer 522, the
residual mask material layer 522 can be removed by a wet etching method using a
diluted hydrofluoric acid aqueous solution.
[Step-2350]
-
Inside the opening portion 514 formed in the insulating layer 512,
the side wall surface of the opening portion 514 is receded under an isotropic
etching condition, whereby an field emission device shown in Fig. 52B is
completed. For the isotropic etching, there can be employed those explained in
the production method in Example 22.
-
Meanwhile, in the electron-emitting portion 15D formed in
Example 23, a sharper conical form is formed than the counterpart in the electron
emitting portion 15D formed in Example 22. This difference is caused by
differences in form of the mask material layers 522 and the ratio of the etching
rate of electrically conductive material layer 521 to the etching rate of the mask
material layer 522. The above differences will be explained with reference to
Figs. 53A and 53B. Figs. 53A and 53B show how the surface profile of a material
being etched changes at constant intervals of time. Fig. 53A shows a case using a
mask material layer 522 composed of copper, and Fig. 53B shows a case using a
mask material layer 522 composed of a resist material. For simplification, it is
assumed that the etching rate of the electrically conductive material layer 521 and
the etching rate of the adhesion layer 520 are the same, and showing of the
adhesion layer 520 is omitted.
-
When the mask material layer 522 composed of copper is used (see
Fig. 53A), the mask material layer 522 disappears in no case during etching since
the etching rate of the mask material layer 522 is sufficiently low as compared
with the etching rate of the electrically conductive material layer 521, so that an
electron-emitting portion having a sharp top end portion can be formed. In
contrast, when a mask material layer 522 composed of a resist material is used
(see Fig. 53B). the mask material layer 522 is liable to disappear during the
etching since the etching rate of the mask material layer 522 is not so high as the
etching rate of the electrically conductive material layer 521. After the mask
material layer disappears, therefore, the conical form of the electron-emitting
portion 15D tends to become obtuse.
-
Further, the mask material layer 522 remaining in the columnar
portion 521B has a merit that the form of the electron-emitting portion 15D does
not much change even if the depth of the columnar portion 521B changes to some
extent. That is, the depth of the columnar portion 521B can vary depending upon
the thickness of the electrically conductive material layer 521 and the fluctuation
of the step coverage. Since, however, the width of the columnar portion 521B is
nearly constant regardless of the depth. the width of the mask material layer 522
comes to be nearly constant, so that there is not much difference in the form of the
electron-emitting portion 15D finally formed. In contrast, in the mask material
layer 522 retained in the recess 521A, the width of the mask material layer
changes depending upon whether the recess has a large depth or a small depth, so
that the conical form of the electron-emitting portion 15D begins to become
obtuse earlier when the recess 521A is shallower and when the mask material
layer 522 has s smaller thickness. The electron emission efficiency of the field
emission device changes depending upon a potential difference between the gate
electrode and the cathode electrode, a distance between the gate electrode and the
cathode electrode and a work function of a material constituting the electron-emitting
portion, and it also changes depending upon the form of top end portion
of the electron emitting portion. It is therefore preferred to make the above
selection of the form and the etching rate of the mask material layer as required.
Example 24
-
Example 24 is a variant of the method of producing the Spindt-type
field emission device of Example 23. In the production method of Example 24, a
nearly funnel-like recess having a columnar portion and a widened portion
communicating with the upper end portion of the columnar portion is formed in a
surface of the electrically conductive material layer in step (e'), the columnar
portion reflecting a step between the upper end surface and the surface of bottom
portion of the opening portion, and in step (f'), the mask material layer is formed
on the entire surface of the electrically conductive material layer, and the mask
material layer on the electrically conductive material layer and inside the widened
portion is removed, whereby the mask material layer is retained in the columnar
portion. The method of producing the Spindt-type field emission device in
Example 24 will be explained hereinafter with reference to Figs. 54A, 54B and 55
showing schematic partial end views of the supporting substrate, etc.
[Step-2400]
-
Procedures up to the formation of the mask material layer 522
shown in Fig. 51A are carried out in the same manner as in [Step-2300] to [Step2320]
in Example 23. and then the mask material layer 522 only on the
electrically conductive material layer 521 and inside the widened portion 521C is
removed, to retain the mask material layer 522 in the columnar portion 521B (see
Fig. 54A). In this case, wet etching is carried out, for example, with a diluted
hydrofluoric acid aqueous solution, whereby only the mask material layer 522
composed of copper can be selectively removed without removing the electrically
conductive material layer 521 composed of tungsten. The height of the mask
material layer 522 remaining in the columnar portion 521B differs depending
upon the etching time period. However, the etching time period is not so strict so
long as the mask material layer 522 filled in the widened portion 521C is fully
removed. The reason therefor is as follows. A discussion on the height of the
mask material layer 522 is substantially the same as the above discussion made on
the depth of the columnar portion 521B with reference to Fig. 53A, and the height
of the mask material layer 522 has no major effect on the form of the electron-emitting
portion 15D to be finally formed.
[Step-2410]
-
Then, the electrically conductive material layer 521, the mask
material layer 522 and the adhesion layer 520 are etched in the same manner as in
Example 23, to form the electron-emitting portion 15D shown in Fig. 54B. While
the electron-emitting portion 15D may naturally have a conical form as a whole as
shown in Fig. 52A, Fig. 54B shows a variant in which a top portion alone has a
conical form. Such a form is produced when the height of the mask material layer
522 filled in the columnar portion 521B is small or when the etching rate of the
mask material layer 522 is relatively high. Such a form does not at all affect the
function of the electron-emitting portion 15D.
[Step-2420]
-
In the opening portion 514 formed in the insulating layer 512, the
side wall surface of the opening portion 514 is receded under an isotropic etching
condition, whereby the field emission device shown in Fig. 55 is completed. The
isotropic etching can be carried out in the same manner as in the production
method explained in Example 22.
Example 25
-
The production method of Example 25 is a variant of the
production method of Example 22. Fig. 56 shows a schematic partial end view in
Example 25. Example 25 differs from Example 22 in that the electron-emitting
portion has a base 530 and a conical electron-emitting portion 15D formed on the
base 530. The base 530 is composed of one material, and the electron-emitting
portion 15D is composed of another material. Specifically, the base 530 is a
member for adjusting a distance between the electron-emitting portion 15D and
the opening end portion of the gate electrode 313, has a function as a resistance
layer and is constituted of a polysilicon layer containing an impurity. The
electron-emitting portion 15D is composed of tungsten, and has a conical form,
more specifically, the form of a circular cone. An adhesion layer 520 composed
of TiN is formed between the base 530 and the electron-emitting portion 15D.
The adhesion layer 520 is not a component essential for the function of the
electron-emitting portion but is provided for a production-related reason. The
insulating layer 512 is scraped from immediately below the gate electrode 313
toward the upper end portion of the base 530. to form an opening portion 514.
-
The production method of Example 25 will be explained
hereinafter with reference to Figs. 57A, 57B, 58A, 58B, 59A and 59B.
[Step-2500]
-
First, procedures up to the formation of the opening portion 514 are
carried out in the same manner as in [Step-2200] in the production method of
Example 22. Then, an electrically conductive material layer 530A for forming the
base is formed on the entire surface including the inside of the opening portion
514. The electrically conductive material layer 530A also works as a resistance
layer, is constituted of a polysilicon layer and can be formed by a plasma CVD
method. Then, a flattening layer 531 constituted of a resist layer is formed on the
entire surface so as to form a nearly flat surface (see Fig. 57A). Then, the
flattening layer 531 and the electrically conductive material layer 530A are etched
under a condition where etching rates of these layers are nearly the same, to fill
part of the opening portion 514 with the base portion 530 having a flat upper
surface (see Fig. 57B). The etching can be carried out by an RIE method using an
etching gas containing a chlorine-containing gas and an oxygen-containing gas.
Since the surface of the electrically conductive material layer 530A is flattened
with the flattening layer 531, the base 530 comes to have a flat upper surface.
[Step-2510]
-
Then, an adhesion layer 520 is formed on the entire surface
including the inside of rest of the opening portion 514, and an electrically
conductive material layer 521 for an electron-emitting portion is formed on the
entire surface including the inside of rest of the opening portion 514, to fill the
rest of the opening portion 514 with the electrically conductive material layer 521
(see Fig. 58A). The adhesion layer 520 is a 0.07 µm thick TiN layer formed by a
sputtering method, and the electrically conductive material layer 521 is a 0.6 µm
thick tungsten layer formed by a reduced pressure CVD method. A recess 521A
reflecting a step between the upper end surface and the surface of bottom portion
of the opening portion 514 is formed in the surface of the electrically conductive
material layer 521.
[Step-2520]
-
Then, a mask material layer 522 constituted of a resist layer is
formed on the entire surface of the electrically conductive material layer 521 by a
spin coating method to form a nearly flat surface (Fig. 58B). The mask material
layer 522 absorbs the recess 521A in the surface of the electrically conductive
material layer 521 and forms a nearly flat surface. Then, the mask material layer
522 is etched by an RIE method using an oxygen gas (see Fig. 59A). The etching
is terminated when a flat surface of the electrically conductive material layer 521
is exposed. In this manner, the mask material layer 522 is retained in the recess
521 A of the electrically conductive material 521 to form a flat surface, and the
mask material layer 522 is formed so as to cover a region of the electrically
conductive material layer 521 which region is positioned in the center of the
opening portion 514.
[Step-2530]
-
Then, the electrically conductive material layer 521, the mask
material layer 522 and the adhesion layer 520 are etched together in the same
manner as in [Step-2240] in the production method of Example 22, whereby the
electron-emitting portion 15D having a conical form depending upon the selective
ratio to a resist based on the above-described mechanism and the adhesion layer
520 are formed, and the electron-emitting portion is completed (see Fig. 59B).
Then, inside the opening portion 514 formed in the insulating layer 512, the side
wall surface of the opening portion 514 is receded, whereby an field emission
device shown in Fig. 56 can be obtained.
Example 26
-
The production method of Example 26 is a variant of the
production method of Example 23. Fig. 61B shows a schematic partial end view
in Example 26. Example 26 differs from Example 23 in that the electron-emitting
portion has a base 530 and a conical electron-emitting portion 15D formed on the
base 530 like the electron-emitting portion in Example 25. The base 530 is
composed of one material, and the electron-emitting portion 15D is composed of
another material. Specifically, the base 530 is a member for adjusting a distance
between the electron-emitting portion 15D and the opening end portion of the gate
electrode 313, has a function as a resistance layer and is constituted of a
polysilicon layer containing an impurity. The electron-emitting portion 15D is
composed of tungsten, and has a conical form, more specifically, the form of a
circular cone. An adhesion layer 520 composed of TiN is formed between the
base 530 and the electron-emitting portion 15D. The adhesion layer 520 is not a
component essential for the function of the electron-emitting portion but is
provided for a production-related reason. The insulating layer 512 is scraped
from immediately below the gate electrode 313 toward the upper end portion of
the base 530, to form an opening portion 514.
-
The production method of Example 26 will be explained
hereinafter with reference to Figs. 60A, 60B, 61A and 61B showing schematic
partial end views of a supporting substrate, etc.
[Step-2600]
-
First, procedures up to the formation of the opening portion 514 are
carried out in the same manner as in [Step-2200] in the production method of
Example 22. Then. an electrically conductive material layer for forming the base
is formed on the entire surface including the inside of the opening portion 514,
and the electrically conductive material layer is etched, whereby the base 530
filling part of the opening portion 514 can be formed. While the base 530 shown
in Figures has a flat surface, the surface may be dented. The base 530 having a
flat surface can be formed in the same manner as in [Step-2500] in the production
method of Example 25. Further, the adhesion layer 520 and the electrically
conductive material layer 521 for an electron-emitting portion are consecutively
formed on the entire surface including the inside of rest of the opening portion
514. In this case, the thickness of the electrically conductive material layer 521 is
determined such that a nearly funnel-like recess 521A having a columnar portion
521B and a widened portion 521C communicating with the upper end portion of
the columnar portion 521B is formed in a surface of the electrically conductive
material layer 521, the columnar portion 521B reflecting a step between the upper
end surface of the rest of the opening portion 514 and the surface of the bottom
portion thereof. Then, the mask material layer 522 is formed on the electrically
conductive material layer 521. The mask material layer 522 is composed, for
example, of copper. Fig. 60A shows the thus-completed state.
[Step-2610]
-
The mask material layer 522 and the electrically conductive
material layer 521 are removed in a plane in parallel with the surface of the
supporting substrate 510, to retain the mask material layer 522 in the columnar
portion 521B (see Fig. 60B). The above removal can be carried out by a chemical
mechanical/polishing method (CMP method) in the same manner as in [Step-2330]
in Example 23.
[Step-2620]
-
Then, the electrically conductive material layer 521, the mask
material layer 522 and the adhesion layer 520 are etched, to form an electron-emitting
portion 15D having a conical form depending upon the selective ratio to
a resist based on the above-described mechanism. These layers can be etched in
the same manner as in [Step-2340] in the production method of Example 23. The
electron-emitting portion comprises the electron-emitting portion 15D, the base
530 and the adhesion layer 520 remaining between the electron-emitting portion
15D and the base 530. While the electron-emitting portion may naturally have a
conical form as a whole, Fig. 61A shows a state where the base 530 is filled in
part of the opening portion 514. Such a form is produced when the mask material
layer 522 filled in the columnar portion 521 has a small height or when the
etching rate of the mask material layer 522 is relatively high. The above form
does not at all affect the function of the electron-emitting portion.
[Step-2630]
-
Then, inside the opening portion 514, the side wall surface of the
insulating layer 512 is receded under an isotropic etching condition, whereby an
field emission device shown in Fig. 61B is completed. The isotropic etching
condition can be the same as those explained in the production method of
Example 22.
Example 27
-
The production method of Example 27 is a variant of the method of
producing the Spindt-type field emission device in Example 24. Example 27
differs from Example 24 in that the electron-emitting portion has a base 530 and a
conical electron-emitting portion 15D formed on the base 530 like Example 25.
The method of producing the Spindt-type field emission device in Example 27
will be explained hereinafter with reference to Fig. 62 showing a schematic partial
end view of a supporting substrate, etc.
[Step-2700]
-
Procedures up to the formation of the mask material layer 522 are
carried out in the same manner as in [Step-2600] in the production method of
Example 26. Then, only the mask material layer 522 on the electrically
conductive material layer 521 and in the widened portion 521C is removed,
thereby to retain the mask material layer 522 in the columnar portion 521B (see
Fig. 62). The mask material layer 522 composed of copper can be selectively
removed without removing the electrically conductive material layer 521
composed of tungsten, for example, by wet etching with a diluted hydrofluoric
acid aqueous solution. Thereafter, all the steps of etching the electrically
conductive material layer 521 and the mask material layer 522, isotropically
etching the insulating layer 512, etc., can be carried out in the same manner as in
the production method of Example 26.
-
The present invention has been explained with reference to
Examples hereinabove, while the present invention shall not be limited thereto.
Particulars of constitutions of the field emission devices and the flat-panel
displays explained in Examples are given as examples and may be altered as
required.
-
Various materials used in the production of the field emission
devices are also give as examples and may be altered as required. While the field
emission devices are explained as embodiments in which one electron-emitting
portion corresponds to one opening portion, there may be employed an
embodiment in which a plurality of electron-emitting portions correspond to one
opening portion or one electron-emitting portion corresponds to a plurality of
opening portions, depending upon the structures of the field emission devices.
Further, there may be employed an embodiment in which a plurality of opening
portions are formed in the gate-electrode-constituting layer, one opening portion
communicating with a plurality of such opening portions is formed in the
insulating layer, and one or a plurality of electron-emitting portions is or are
formed.
-
The method of driving the flat-panel display shall not be limited to
the method explained in Examples. Further, the form of the gate electrode or the
electrically conductive material layer for a gate electrode shall not be limited to
the form of a stripe. There may be employed a constitution in which all the gate
electrodes constituting the first panel P1 of the flat-panel display are constituted of
one sheet-like electrode-constituting layer (for example, a single-layered structure
composed of a gas-trapping material or a stacked structure formed of a first layer
composed of an electrically conductive material or an electrically insulating
material and a second layer (gas-trapping layer) composed of a gas-trapping
material). In such constitutions, the cathode electrode has, for example, a
rectangular plan form corresponding to one pixel. In some cases, it is not required
to provide a spacer per cold cathode field emission device.
-
Fig. 63 shows a circuit for driving the above-constituted flat-panel
display. The circuit has a control circuit 30 electrically connected to the electron-emitting
portions (more specifically, the cathode electrodes 11) and a gate-electrode
control circuit (not shown) electrically connected to the gate electrodes
313. Further, the control circuit 30 has a data circuit 130A and a scanning circuit
130B. Each cathode electrode 11 is electrically connected to the data circuit 130A
through a switching element 130C constituted of a MOS transistor. The gate
portion of the MOS transistor is electrically connected to the scanning circuit
130B. The MOS transistor is, for example, an n-channel type MOS transistor and
works as a switching element which controls ON and OFF depending upon
control signals applied from the scanning circuit 130B and the data circuit 130A.
When the switching element 130C comes to be in an ON state, a voltage
depending upon the control signals applied from the scanning circuit 130B and the
data circuit 130A is applied to the cathode electrode 11 electrically connected to
the switching element 130C. The MOS transistor may be constituted of a p-channel
type MOS transistor. Further, the MOS transistor may be replaced with
other switching means having the switching function equivalent to that of the
MOS transistor.
-
The field emission devices arranged in the row direction (X
direction) are consecutively driven in the column direction (Y direction).
Specifically, a constant voltage VG is applied to one sheet-like gate-electrode-constituting
layer having the gate electrodes 313 from the gate-electrode control
circuit. A desired switching element 130C is brought into an ON state with the
control circuit 30, thereby to apply a voltage of 0 ≤ [VC-MAX to VC-MIN] (<VG) to
each cathode electrode 11. In an electron-emitting region having the gate
electrode 313 to which the voltage VG is applied and each cathode electrode 11 to
which the voltage of 0 ≤ [VC-MAX to VC-MIN] is applied, a potential difference ΔV
is the maximum when (VG - VC-MIN), and the quantity of electrons emitted from
the electron-emitting region is the largest, and the electrons are attracted to the
anode electrode 23 to collide with the fluorescent layer 21. As a result, the
fluorescent layer corresponding to such an electron-emitting region has the largest
light emission brightness. On the other hand, when (VG - VC-MAX), the potential
difference ΔV is the smallest, no electrons are emitted from the electron-emitting
region, and the fluorescent layer corresponding to such an electron-emitting
region does not emit light. The light emission brightness of the fluorescent layer
can be controlled by applying a voltage of VC-MAX to VC-MIN to the electrically
conductive material layers for a cathode electrode.
-
Otherwise, there may be employed a constitution in which all of the
cathode electrodes constituting the first panel P1 of the flat-panel display are
constituted of one sheet-like electrically conductive material layer and the gate
electrode 313 is constituted of an electrically conductive material layer in the form
of a stripe. That is, the gate electrode 313 has, for example, a rectangular plan
form corresponding to one pixel. As shown in Fig. 64, a circuit for driving the
flat-panel display can comprise a cathode-electrode control circuit (not shown)
electrically connected to the electron-emitting portions (specifically, the cathode
electrodes) and a control circuit 31 electrically connected to the gate electrodes
313. The control circuit 31 has a data circuit 131A and a scanning circuit 131B.
The gate electrode 313 is electrically connected to the data circuit 13 IA through a
switching element 131C constituted of a MOS transistor. The gate portion of the
MOS transistor is electrically connected to the scanning circuit 131B. The MOS
transistor is, for example, an n-channel type MOS transistor, and works as a
switching element which controls ON and OFF depending upon control signals
applied from the scanning circuit 131B and the data circuit 131A. When the
switching element 131C is brought into an ON state, a voltage depending upon the
control signals applied from the scanning circuit 131B and the data circuit 131A is
applied to the gate electrode 313 electrically connected to the switching element
131C. The MOS transistor may be constituted of a p-channel type MOS
transistor. Further, the MOS transistor may be replaced with other switching
means having the switching function equivalent to that of the MOS transistor.
-
In the above flat-panel display, the field emission devices arranged
in the row direction (X direction) are consecutively driven in the column direction
(Y direction). Specifically, a constant voltage VC is applied to one sheet-like
cathode-electrode-constituting layer having the cathode electrodes 11 from the
cathode-electrode control circuit. A desired switching element 131C is brought
into an ON state with the control circuit 31, thereby to apply a voltage of VC ≤
[VG-MAX to VG-MIN] to each gate electrode 313. In an electron-emitting region
having the cathode electrode 11 to which the voltage VC is applied and each gate
electrode 313 to which the voltage of VG.MAX to VG-MIN is applied, a potential
difference ΔV is the maximum when (VG-MAX - VC), and the quantity of electrons
emitted from the electron-emitting region is the largest, and the electrons are
attracted to the anode electrode 23 to collide with the fluorescent layer 21. As a
result, the fluorescent layer corresponding to such an electron-emitting region has
the largest light emission brightness. On the other hand, when (VG-MIN - VC), the
potential difference ΔV is the smallest, no electrons are emitted from the electron-emitting
region, and the fluorescent layer corresponding to such an electron-emitting
region does not emit light. The light emission brightness of the
fluorescent layer can be controlled by applying a voltage of VG-MAX to VG-MIN to
the gate electrodes 13.
-
Further, the electron-emitting region can be also constituted of
devices generally called surface conduction type field emission devices. The
surface conduction type field emission device comprises a substrate made of a
glass and pairs of electrodes formed on the substrate in the form of matrix, the
electrodes being composed of an electrically conductive material such as tin oxide
(SnO2), gold (Au), indium oxide (In2O3)/tin oxide (SnO2), carbon or palladium
oxide (PdO), having a fine area and a pair of electrodes being arranged at constant
intervals (gaps). A carbon thin film is formed on each electrode. A row-direction
wiring is connected to one electrode of a pair of the electrodes, and a columndirection
wiring is connected to the other electrode. When a voltage is applied to
a pair of the electrodes, an electric field is applied to the carbon thin films
opposed to each other through the gap, and electrons are emitted from the carbon
thin film. Such electrons are allowed to collide with a fluorescent layer on a
second panel (anode panel) to excite the fluorescent layer, whereby a desired
image can be obtained.
-
In Examples, while the focus electrode 47 or 147 is provided above
the gate electrode through the second insulating layer 46. a focus electrode 247
may be provided above the gate electrode through a vacuum layer. In this case,
the focus electrode 247 can substantially have the same structure as that of the
focus electrode 147 in Example 10. Further, a gate electrode 313 can be
structured as explained in Examples of the present invention, or it may have a
conventional structure in some cases. The focus electrode 247 can be composed,
for example, of one sheet-like material. The above focus electrode 247 is fixed to
the second panel P2 through a supporting member 248 arranged in a
circumferential portion of the second panel P2. The focus electrode 247 may have
a single-layered structure composed of a gas-trapping material (composed, for
example, of a titanium alloy having a thickness of 50 µm) or may have a stacked
structure constituted, at least, of a first layer composed of an electrically
conductive material or an electrically insulating material and a second layer
composed of a gas-trapping material. Specifically, the latter can have a
constitution similar to the constitution of the gate electrode explained with
reference to Figs. 19A, 19B, 20A, 20B and 20C. When the focus electrode 247
has a stacked structure, it is preferred to arrange the second layer composed of a
gas-trapping material on the cathode electrode side from the viewpoint that the
vacuum state around the cathode electrode 11 is maintained under a better
condition. That is. it is preferred to reverse the stacking order of the first layer
113A and the second layer 113B in Figs. 19A, 20A, 20B and 20C. In the focus
electrode 247, an opening portion may be formed per field emission device, or
one opening portion may be formed per a plurality of (for example, per pixel) of
field emission devices.
-
As is clear from the above explanations, the getter of the present
invention has a large effective area for exhibiting a gas-trapping effect and can
achieve excellent gas-trapping efficiency over any conventional getter. In the flat-panel
display of the present invention, the getter is provided in at least one of the
first panel and the second panel, so that the gas-trapping efficiency is improved as
compared with any conventional flat-panel display having a getter in one place of
the ineffective field. As a result, the flat-panel display is remarkably improved in
lifetime and image quality. Gas, etc., released into the vacuum layer are trapped
in the gate electrode, the focus electrode or the getter, and a high vacuum
atmosphere can be maintained in the vacuum layer. Even if gas molecules, ions,
etc., are released, for example, from the fluorescent layer, therefore, these are
trapped in the gate electrode, the focus electrode or the getter, so that the collision
thereof with the electron-emitting portions can be prevented. As a result, the
occurrence of local discharging can be prevented, or a change in work function on
the surface of the electron-emitting portion or the deterioration of the electron-emitting
portions can be prevented, so that the electron-emitting portions can be
imparted with a longer lifetime and that the performance can be stabilized by
preventing the deterioration of image display. Further, since a conventional getter
box is no longer necessary, the structure of a flat-panel display can be simplified.
In the production method according to the third or fourth constitution of the
present invention, the gate electrode or the focus electrode of the cold cathode
field emission device is formed to have a pattern different from the pattern of the
getter, the effective area of the getter can be further increased.