WO2009078522A1 - Field emission type back light unit - Google Patents
Field emission type back light unit Download PDFInfo
- Publication number
- WO2009078522A1 WO2009078522A1 PCT/KR2008/003932 KR2008003932W WO2009078522A1 WO 2009078522 A1 WO2009078522 A1 WO 2009078522A1 KR 2008003932 W KR2008003932 W KR 2008003932W WO 2009078522 A1 WO2009078522 A1 WO 2009078522A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- substrate
- metal gate
- field emission
- back light
- light unit
- Prior art date
Links
- 239000000758 substrate Substances 0.000 claims abstract description 113
- 229910052751 metal Inorganic materials 0.000 claims abstract description 71
- 239000002184 metal Substances 0.000 claims abstract description 71
- 239000000463 material Substances 0.000 claims abstract description 49
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 claims abstract description 10
- 125000006850 spacer group Chemical group 0.000 claims description 5
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 claims description 3
- 239000002134 carbon nanofiber Substances 0.000 claims description 2
- 239000002041 carbon nanotube Substances 0.000 claims description 2
- 229910021393 carbon nanotube Inorganic materials 0.000 claims description 2
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 claims description 2
- 229920002994 synthetic fiber Polymers 0.000 claims description 2
- 238000010894 electron beam technology Methods 0.000 description 15
- 239000012212 insulator Substances 0.000 description 8
- 238000009825 accumulation Methods 0.000 description 7
- 230000015572 biosynthetic process Effects 0.000 description 3
- 239000004020 conductor Substances 0.000 description 3
- 230000001939 inductive effect Effects 0.000 description 2
- 239000004973 liquid crystal related substance Substances 0.000 description 2
- 238000001459 lithography Methods 0.000 description 2
- 239000000395 magnesium oxide Substances 0.000 description 2
- CPLXHLVBOLITMK-UHFFFAOYSA-N magnesium oxide Inorganic materials [Mg]=O CPLXHLVBOLITMK-UHFFFAOYSA-N 0.000 description 2
- AXZKOIWUVFPNLO-UHFFFAOYSA-N magnesium;oxygen(2-) Chemical compound [O-2].[Mg+2] AXZKOIWUVFPNLO-UHFFFAOYSA-N 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000010409 thin film Substances 0.000 description 2
- 230000001133 acceleration Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 238000005136 cathodoluminescence Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- AMGQUBHHOARCQH-UHFFFAOYSA-N indium;oxotin Chemical compound [In].[Sn]=O AMGQUBHHOARCQH-UHFFFAOYSA-N 0.000 description 1
- 239000007769 metal material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- YVTHLONGBIQYBO-UHFFFAOYSA-N zinc indium(3+) oxygen(2-) Chemical compound [O--].[Zn++].[In+3] YVTHLONGBIQYBO-UHFFFAOYSA-N 0.000 description 1
- TYHJXGDMRRJCRY-UHFFFAOYSA-N zinc indium(3+) oxygen(2-) tin(4+) Chemical compound [O-2].[Zn+2].[Sn+4].[In+3] TYHJXGDMRRJCRY-UHFFFAOYSA-N 0.000 description 1
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
- G02F1/1336—Illuminating devices
- G02F1/133617—Illumination with ultraviolet light; Luminescent elements or materials associated to the cell
-
- G—PHYSICS
- G02—OPTICS
- G02F—OPTICAL DEVICES OR ARRANGEMENTS FOR THE CONTROL OF LIGHT BY MODIFICATION OF THE OPTICAL PROPERTIES OF THE MEDIA OF THE ELEMENTS INVOLVED THEREIN; NON-LINEAR OPTICS; FREQUENCY-CHANGING OF LIGHT; OPTICAL LOGIC ELEMENTS; OPTICAL ANALOGUE/DIGITAL CONVERTERS
- G02F1/00—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics
- G02F1/01—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour
- G02F1/13—Devices or arrangements for the control of the intensity, colour, phase, polarisation or direction of light arriving from an independent light source, e.g. switching, gating or modulating; Non-linear optics for the control of the intensity, phase, polarisation or colour based on liquid crystals, e.g. single liquid crystal display cells
- G02F1/133—Constructional arrangements; Operation of liquid crystal cells; Circuit arrangements
- G02F1/1333—Constructional arrangements; Manufacturing methods
- G02F1/1335—Structural association of cells with optical devices, e.g. polarisers or reflectors
- G02F1/1336—Illuminating devices
- G02F1/133602—Direct backlight
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J3/00—Details of electron-optical or ion-optical arrangements or of ion traps common to two or more basic types of discharge tubes or lamps
- H01J3/02—Electron guns
- H01J3/021—Electron guns using a field emission, photo emission, or secondary emission electron source
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J63/00—Cathode-ray or electron-stream lamps
- H01J63/02—Details, e.g. electrode, gas filling, shape of vessel
Definitions
- the present invention relates to a field emission display, and more particularly, to a field emission-back light unit having improved field emission efficiency.
- flat panel displays may be classified into emissive displays and non- emissive displays.
- the emissive displays include a plasma display panel (PDP) and a field emission display (FED), and the non-emissive displays include a liquid crystal display (LCD).
- PDP plasma display panel
- FED field emission display
- LCD liquid crystal display
- the LCD has advantages of light weight and low power consumption, it cannot create an image by self-emission, but only by light entering from outside. Thus, the image created by the LCD cannot be observed in a dark place.
- a back light unit is installed at a back surface of the LCD.
- a cold cathode fluorescent lamp which is a linear light source
- a light emitting diode which is a spot light source
- a cathode substrate having a field emitter and an anode substrate having a phosphor are disposed to face and be spaced a specific distance apart from each other, and vacuum-packed.
- An electron emitted from the field emitter collides with the phosphor of the anode substrate, so that light is emitted by cathodoluminescence of the phosphor.
- FIG. 1 illustrates a conventional field emission device having a top-gate triode structure.
- the field emission device using a dielectric thin film as a gate insulator 102 may have an emitter 104 formed by printing after formation of a gate and may be easily surfaced- treated, because of a low-height gate insulator 102.
- the emitter 104 and an electrode structure may be damaged due to occurrence of arc, and a production cost increases due to necessity of lithography.
- the field emission device having a structure as in FIG. Ib is less likely to be damaged by the arc, so that a high voltage can be relatively easily applied thereto.
- the field emission device having a structure as in FIG. Ib has to have an emitter 104 and be surfaced- treated before formation of a gate structure, and an electron emitted from the emitter 104 collides with the gate insulator 102 to cause the charge accumulation.
- an aperture ratio i.e., a ratio of a gate hole to the total area of the device.
- it is not easy to increase the aperture ratio because of a ratio of a diameter of a gate opening to a height of a gate insulator and a structural characteristic of a gate electrode.
- the present invention is directed to a field emission-back light unit having high field emission efficiency.
- One aspect of the present invention provides a field emission-back light unit, including: an upper substrate and a lower substrate, which are spaced apart from and face each other; an anode electrode and a phosphor layer, which are formed on the upper substrate; a cathode electrode formed on the lower substrate; a plurality of field emitters formed on the cathode electrode and spaced apart from one another; and a metal gate substrate disposed between the upper substrate and the lower substrate to induce electron emission from the field emitter, and having an opening through which the emitted electron passes, wherein at least one surface of the metal gate substrate is coated with a secondary electron-generating material capable of generating secondary electrons by collision of the emitted electrons.
- the present invention can improve field emission efficiency with a secondary electron, which is generated from a secondary electron-generating material coated on a metal gate substrate inducing electron emission.
- FIG. 1 illustrates a conventional field emission device having a top-gate triode structure
- FIG. 2 is a schematic view of a field emission-back light unit according to an exemplary embodiment of the present invention.
- FIGS. 3 to 6 illustrate generation of secondary electrons depending on shapes of an opening formed in a metal gate substrate according to exemplary embodiments of the present invention.
- a conventional field emission device having a top-gate triode structure and used as a back light for a liquid crystal display has a gate structure using a dielectric thin film or a dielectric substrate as an insulator, and has problems of damage of an electrode structure due to arc occurring in application of high voltage, and an increase in production cost caused by a lithography process.
- the present invention provides a field emission-back light unit which is easily formed in a large size and has high field emission efficiency by using a metal substrate having an opening through which an electron beam emitted from an emitter can pass as a gate electrode, and the gate electrode coated with a material for facilitating generation of a secondary electron so as to generate the secondary electron due to collision of some electron beams emitted from the emitter with the material.
- FIG. 2 is a schematic view of a field emission-back light unit according to an exemplary embodiment of the present invention.
- the field emission-back light unit according to the exemplary embodiment of the present invention includes a lower substrate 210 as a cathode substrate, a cathode electrode 212 formed on the lower substrate 210, a field emitter 214 formed on the cathode electrode 212, an upper substrate 220 as an anode substrate, an anode electrode 222 formed on the upper substrate 220, a phosphor layer 224 formed on the anode electrode 222, a metal gate substrate 232 coated with a secondary electron-generating material 234, and spacers 242 and 244.
- the lower substrate 210 is spaced apart from and faces the upper substrate 220, and maintains a specific distance therebetween by the spacer 242 formed between the lower substrate 210 and the metal gate substrate 232, and the spacer 244 formed between the upper substrate 220 and the metal gate substrate 232.
- the lower substrate 210 and the upper substrate 220 may be glass substrates.
- the cathode electrode 212 may be formed on the lower substrate 210, and formed of a metallic material or a transparent conductive material.
- the transparent conductive material may be indium tin oxide (ITO), indium zinc oxide (IZO) or indium tin zinc oxide (ITZO).
- At least one field emitter 214 is formed on the cathode electrode 212, and preferably, a plurality of field emitters 214 are formed to be spaced a specific distance apart from one another.
- the field emitter 214 may be formed of an electron emission material having an excellent electron emission characteristic, which includes a carbon nano tube, a carbon nano fiber and a carbon-based synthetic material.
- the anode electrode 222 is formed on the upper substrate 220, and the phosphor layer 224 is disposed on the anode electrode 222.
- the anode electrode 222 may also be formed of a transparent conductive material, such as ITO, IZO or ITZO.
- the metal gate substrate 232 serves as a gate electrode inducing electron emission from the field emitter 214, and maintains a specific distance apart from the upper and lower substrates 220 and 210 by the spacers 242 and 244.
- a plurality of openings 236 are formed in the metal gate substrate 232, wherein the opening 236 may be formed to correspond to a location of the field emitter 214.
- the secondary electron-generating material 234 which facilitates the generation of a secondary electron due to collision of electron beams emitted from the field emitter 214 is coated on at least one surface of the metal gate substrate 232. While FIG. 2 shows that the secondary electron-generating material 234 is coated on a bottom surface of the metal gate substrate 232 and a side surface thereof adjacent to the opening 236, the secondary electron-generating material 234 may be also coated on a top surface of the metal gate substrate 232, if necessary. Further, to generate more secondary electrons due to the collision of the electron beams, a width of the field emitter 214 may be formed larger than a diameter of the opening 236.
- the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236.
- the secondary electron-generating material 235 may include magnesium oxide (MgO).
- the secondary electron generated as such is combined with an electron emitted from the field emitter 214, and the combined result passes through the opening 236 and collides with the phosphor layer 224, such that light is emitted.
- 232 may be coated as thin as possible to prevent the accumulation of charges.
- FIG. 3 illustrates generation of secondary electrons in a metal gate substrate having an opening with a rectangular longitudinal-section according to an exemplary embodiment of the present invention.
- an opening 236 with a rectangular longitudinal- section is formed in a metal gate substrate 232, and a secondary electron-generating material 234 is coated on a side surface of the metal gate substrate 232 adjacent to the opening 236 and a bottom surface of the metal gate substrate 232.
- Some electron beams 301 i.e., the flow of electrons emitted from a field emitter 214, pass through the opening 236 without collision with the metal gate substrate 232, and the other electron beams collide with the secondary electron-generating material 234 coated on the metal gate substrate 232 so as to generate secondary electrons e.
- the secondary electrons e generated as such pass through the opening 236 together with the electron beams emitted from the field emitter 214, and go to an anode electrode.
- the secondary electron-generating material 234 may be coated only on a side surface of the metal gate substrate 232 adjacent to the opening 236, or only on a bottom surface of the metal gate substrate 232.
- the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening
- FIG. 4 illustrates generation of secondary electrons in a metal gate substrate having an opening with a reverse-tapered longitudinal-section according to another exemplary embodiment of the present invention.
- an opening 236 with a reverse-tapered longitudinal- section may be formed in a metal gate substrate 232, and a secondary electron-generating material
- the metal gate substrate 232 is coated on a bottom surface of the metal gate substrate 232.
- some electron beams 301 i.e., the flow of electrons emitted from a field emitter 214, pass through the opening 236 without collision with the metal gate substrate 232, and the other electron beams collide with the secondary electron-generating material 234 coated on the metal gate substrate 232 and generate secondary electrons e.
- an area of a side surface of the metal gate substrate 232 on which the secondary electron-generating material 234 is coated is larger, so that more secondary electrons e can be generated.
- the secondary electron-generating material 234 may be coated only on a side surface of the metal gate substrate 232 adjacent to the opening 236, or only on a bottom surface of the metal gate substrate 232.
- the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 4b.
- the secondary electron-generating material 234 may be coated on bottom and top surfaces of the gate substrate 232, and the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 4c.
- a width of the filed emitter 214 may be formed larger than a diameter of the opening
- FIG. 5 illustrates generation of secondary electrons in a metal gate substrate having an opening with a tapered longitudinal- section according to still another exemplary embodiment of the present invention.
- an opening 236 with a tapered longitudinal-section may be formed in a metal gate substrate 232, and a secondary electron-generating material 234 may be coated on a bottom surface of the metal gate substrate 232, and a side surface of the metal gate substrate 232 adjacent to the opening 236.
- some electron beams 301 i.e., the flow of electrons emitted from a field emitter 214, pass through the opening 236 without collision with the metal gate substrate 232, and the other electron beams collide with the secondary electron-generating material 234 coated on the metal gate substrate 232, and generate secondary electrons e.
- the structure of FIG. 5a can reduce a loss of electron beams which leak through the metal gate substrate 232.
- the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236, or only on the bottom surface of the metal gate substrate 232.
- the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 5b.
- the secondary electron-generating material 234 may be coated on the bottom and top surfaces of the metal gate substrate 232, and the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 5c.
- a width of the field emitter 214 may be formed larger than a diameter of the opening
- FIG. 6 illustrates generation of secondary electrons in a metal gate substrate having an opening with a longitudinal-section which has a tapered lower region, and a reverse- tapered upper region according to yet another exemplary embodiment of the present invention.
- a metal gate substrate 232 has an opening 236 with a longitudinal-section having a tapered lower region and a reverse-tapered upper region, and a secondary electron-generating material 234 is coated on a bottom surface of the metal gate substrate 232 and a side surface thereof adjacent to the tapered lower region of the opening 236.
- some electron beams 301 i.e., the flow of electrons emitted from a field emitter 214 pass through an opening 236 without collision with the metal gate substrate 232, and the other electron beams collide with the secondary electron-generating material 234 coated on the metal gate substrate 232 and generate secondary electrons e.
- the structure of FIG. 6a described above can reduce a loss of electron beams which leak through the metal gate substrate 232, like the structure of FIG. 5a.
- the structure of FIG. 6a facilitates the flow of the generated electrons e to an anode, compared to the structure of FIG. 5a.
- the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236, or only on the bottom surface of the metal gate substrate 232.
- the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 6b.
- the secondary electron-generating material 234 may be coated on the bottom and top surfaces of the metal gate substrate 232, and the side surface thereof adjacent to the opening 236, which is illustrated in FIG. 6c.
- a width of the field emitter 214 may be formed larger than a diameter of the opening
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- Mathematical Physics (AREA)
- Chemical & Material Sciences (AREA)
- Crystallography & Structural Chemistry (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Cold Cathode And The Manufacture (AREA)
- Cathode-Ray Tubes And Fluorescent Screens For Display (AREA)
Abstract
A field emission display, more particularly, a field emission-back light unit having high field emission efficiency is provided. The field emission-back light unit includes an upper substrate and a lower substrate, which are spaced apart from and face each other, an anode electrode and a phosphor layer, which are formed on the upper substrate, a cathode electrode formed on the lower substrate, a plurality of field emitters formed on the cathode electrode and spaced apart from one another, and a metal gate substrate disposed between the upper substrate and the lower substrate to induce electron emission from the field emitter, and having an opening through which the emitted electron passes. At least one surface of the metal gate substrate is coated with a secondary electron-generating material capable of generating secondary electrons by collision of the emitted electrons.
Description
Description FIELD EMISSION TYPE BACK LIGHT UNIT
Technical Field
[I] The present invention relates to a field emission display, and more particularly, to a field emission-back light unit having improved field emission efficiency. Background Art
[2] Generally, flat panel displays may be classified into emissive displays and non- emissive displays.
[3] The emissive displays include a plasma display panel (PDP) and a field emission display (FED), and the non-emissive displays include a liquid crystal display (LCD).
[4] While the LCD has advantages of light weight and low power consumption, it cannot create an image by self-emission, but only by light entering from outside. Thus, the image created by the LCD cannot be observed in a dark place. To solve this problem, a back light unit is installed at a back surface of the LCD.
[5] Conventionally, as a back light unit, a cold cathode fluorescent lamp (CCFL), which is a linear light source, and a light emitting diode (LED), which is a spot light source, are mainly used.
[6] However, such back light units are complicated and expensive, and consume a large amount of power according to reflection and transmission of light due to the light source disposed at a side thereof. Particularly, as the LCD becomes larger, uniform brightness becomes difficult to ensure.
[7] For these reasons, in recent time, a field emission-back light unit having a flat emission structure has been developed. Such a field emission-back light unit consumes less power and exhibits relatively uniform brightness in a wide range of an emission region, compared to the conventional back light unit using a CCFL.
[8] Generally, in a field emission-back light unit, a cathode substrate having a field emitter and an anode substrate having a phosphor are disposed to face and be spaced a specific distance apart from each other, and vacuum-packed. An electron emitted from the field emitter collides with the phosphor of the anode substrate, so that light is emitted by cathodoluminescence of the phosphor.
[9] A structure of the conventional field emission device will now be described with reference to FIG. 1.
[10] FIG. 1 illustrates a conventional field emission device having a top-gate triode structure.
[I I] Referring to FIG. Ia, the field emission device using a dielectric thin film as a gate insulator 102 may have an emitter 104 formed by printing after formation of a gate and
may be easily surfaced- treated, because of a low-height gate insulator 102. However, the emitter 104 and an electrode structure may be damaged due to occurrence of arc, and a production cost increases due to necessity of lithography.
[12] To solve these problems, a field emission device having a high-height gate insulator
102 formed of a thick dielectric or a dielectric mash substrate as in FIG. Ib was developed. The field emission device having a structure as in FIG. Ib is less likely to be damaged by the arc, so that a high voltage can be relatively easily applied thereto. However, the field emission device having a structure as in FIG. Ib has to have an emitter 104 and be surfaced- treated before formation of a gate structure, and an electron emitted from the emitter 104 collides with the gate insulator 102 to cause the charge accumulation. Moreover, it is difficult to form a thick gate insulator 102 in formation of a large-sized device.
[13] In addition, in order to improve efficiency, brightness and uniformity of the field emission device having the top-gate triode structure described above, an aperture ratio, i.e., a ratio of a gate hole to the total area of the device, should be increased. However, it is not easy to increase the aperture ratio because of a ratio of a diameter of a gate opening to a height of a gate insulator and a structural characteristic of a gate electrode.
[14] Thus, a field emission-back light unit which has high field emission efficiency and can be easily formed in a larger size is needed. Disclosure of Invention
Technical Problem
[15] The present invention is directed to a field emission-back light unit having high field emission efficiency.
[16] Other objects of the present invention will be understood with reference to the following descriptions and exemplary embodiments of the present invention. Technical Solution
[17] One aspect of the present invention provides a field emission-back light unit, including: an upper substrate and a lower substrate, which are spaced apart from and face each other; an anode electrode and a phosphor layer, which are formed on the upper substrate; a cathode electrode formed on the lower substrate; a plurality of field emitters formed on the cathode electrode and spaced apart from one another; and a metal gate substrate disposed between the upper substrate and the lower substrate to induce electron emission from the field emitter, and having an opening through which the emitted electron passes, wherein at least one surface of the metal gate substrate is coated with a secondary electron-generating material capable of generating secondary electrons by collision of the emitted electrons.
Advantageous Effects
[18] As described above, the present invention can improve field emission efficiency with a secondary electron, which is generated from a secondary electron-generating material coated on a metal gate substrate inducing electron emission. Brief Description of the Drawings
[19] FIG. 1 illustrates a conventional field emission device having a top-gate triode structure;
[20] FIG. 2 is a schematic view of a field emission-back light unit according to an exemplary embodiment of the present invention; and
[21] FIGS. 3 to 6 illustrate generation of secondary electrons depending on shapes of an opening formed in a metal gate substrate according to exemplary embodiments of the present invention. Mode for the Invention
[22] In the following description, it is to be noted that a detailed description of the known function and configuration of the present invention will be omitted if it is deemed to obscure the subject matter of the present invention. The terms described below, as terms defined considering their functions in the present invention, can be different depending on a user or operator s intention, or a practice. Thus, the definition should be made on the basis of the contents throughout this specification.
[23] In general, a conventional field emission device having a top-gate triode structure and used as a back light for a liquid crystal display has a gate structure using a dielectric thin film or a dielectric substrate as an insulator, and has problems of damage of an electrode structure due to arc occurring in application of high voltage, and an increase in production cost caused by a lithography process. To solve these problems, the present invention provides a field emission-back light unit which is easily formed in a large size and has high field emission efficiency by using a metal substrate having an opening through which an electron beam emitted from an emitter can pass as a gate electrode, and the gate electrode coated with a material for facilitating generation of a secondary electron so as to generate the secondary electron due to collision of some electron beams emitted from the emitter with the material.
[24] Hereinafter, exemplary embodiments of the present invention will be described with reference to the accompanying drawings in detail.
[25] FIG. 2 is a schematic view of a field emission-back light unit according to an exemplary embodiment of the present invention. Referring to FIG. 2, the field emission-back light unit according to the exemplary embodiment of the present invention includes a lower substrate 210 as a cathode substrate, a cathode electrode 212 formed on the lower substrate 210, a field emitter 214 formed on the cathode electrode 212, an upper substrate 220 as an anode substrate, an anode electrode 222
formed on the upper substrate 220, a phosphor layer 224 formed on the anode electrode 222, a metal gate substrate 232 coated with a secondary electron-generating material 234, and spacers 242 and 244.
[26] The lower substrate 210 is spaced apart from and faces the upper substrate 220, and maintains a specific distance therebetween by the spacer 242 formed between the lower substrate 210 and the metal gate substrate 232, and the spacer 244 formed between the upper substrate 220 and the metal gate substrate 232. The lower substrate 210 and the upper substrate 220 may be glass substrates.
[27] The cathode electrode 212 may be formed on the lower substrate 210, and formed of a metallic material or a transparent conductive material. The transparent conductive material may be indium tin oxide (ITO), indium zinc oxide (IZO) or indium tin zinc oxide (ITZO).
[28] At least one field emitter 214 is formed on the cathode electrode 212, and preferably, a plurality of field emitters 214 are formed to be spaced a specific distance apart from one another.
[29] The field emitter 214 may be formed of an electron emission material having an excellent electron emission characteristic, which includes a carbon nano tube, a carbon nano fiber and a carbon-based synthetic material.
[30] The anode electrode 222 is formed on the upper substrate 220, and the phosphor layer 224 is disposed on the anode electrode 222. The anode electrode 222 may also be formed of a transparent conductive material, such as ITO, IZO or ITZO.
[31] The metal gate substrate 232 serves as a gate electrode inducing electron emission from the field emitter 214, and maintains a specific distance apart from the upper and lower substrates 220 and 210 by the spacers 242 and 244.
[32] A plurality of openings 236 are formed in the metal gate substrate 232, wherein the opening 236 may be formed to correspond to a location of the field emitter 214.
[33] The secondary electron-generating material 234 which facilitates the generation of a secondary electron due to collision of electron beams emitted from the field emitter 214 is coated on at least one surface of the metal gate substrate 232. While FIG. 2 shows that the secondary electron-generating material 234 is coated on a bottom surface of the metal gate substrate 232 and a side surface thereof adjacent to the opening 236, the secondary electron-generating material 234 may be also coated on a top surface of the metal gate substrate 232, if necessary. Further, to generate more secondary electrons due to the collision of the electron beams, a width of the field emitter 214 may be formed larger than a diameter of the opening 236. In addition, to prevent accumulation of charges in the secondary electron-generating material 234 having general insulator s characteristics, the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to
the opening 236. Meanwhile, the secondary electron-generating material 235 may include magnesium oxide (MgO).
[34] An emission mechanism of the field emission-back light unit having the above- described structure according to the exemplary embodiment of the present invention will now be described.
[35] Some electrons emitted form the field emitter 214 pass through the opening 236 and collide with the phosphor layer 224, and the others emitted collide with the secondary electron-generating material 234 coated on the metal gate substrate 232 and generate secondary electrons. Here, more secondary electrons are generated according to an acceleration voltage between a gate and a cathode.
[36] The secondary electron generated as such is combined with an electron emitted from the field emitter 214, and the combined result passes through the opening 236 and collides with the phosphor layer 224, such that light is emitted.
[37] In the structure described above, secondary electrons are generated using electrons which leak through a gate electrode, i.e., the metal gate substrate 232, so that an amount of electrons passing through the opening 236 is increased, and thus emission efficiency is improved.
[38] Here, the secondary electron-generating material coated on the metal gate substrate
232 may be coated as thin as possible to prevent the accumulation of charges.
[39] FIG. 3 illustrates generation of secondary electrons in a metal gate substrate having an opening with a rectangular longitudinal-section according to an exemplary embodiment of the present invention.
[40] Referring to FIG. 3a, an opening 236 with a rectangular longitudinal- section is formed in a metal gate substrate 232, and a secondary electron-generating material 234 is coated on a side surface of the metal gate substrate 232 adjacent to the opening 236 and a bottom surface of the metal gate substrate 232.
[41] Some electron beams 301, i.e., the flow of electrons emitted from a field emitter 214, pass through the opening 236 without collision with the metal gate substrate 232, and the other electron beams collide with the secondary electron-generating material 234 coated on the metal gate substrate 232 so as to generate secondary electrons e.
[42] The secondary electrons e generated as such pass through the opening 236 together with the electron beams emitted from the field emitter 214, and go to an anode electrode.
[43] If necessary, the secondary electron-generating material 234 may be coated only on a side surface of the metal gate substrate 232 adjacent to the opening 236, or only on a bottom surface of the metal gate substrate 232.
[44] Here, to prevent accumulation of charges in the secondary electron-generating material 234 as descried above, the secondary electron-generating material 234 may be
coated only on the side surface of the metal gate substrate 232 adjacent to the opening
236, which is illustrated in FIG. 3b. [45] Alternatively, the secondary electron-generating material 234 may be coated on the bottom and top surfaces of the metal gate substrate 232, and the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 3c. [46] To generate more secondary electrons e, a width of the field emitter 214 may be formed larger than a diameter of the opening 236, which is not dependant on a location of the secondary electron-generating material 234. [47] FIG. 4 illustrates generation of secondary electrons in a metal gate substrate having an opening with a reverse-tapered longitudinal-section according to another exemplary embodiment of the present invention. [48] Referring to FIG. 4a, an opening 236 with a reverse-tapered longitudinal- section may be formed in a metal gate substrate 232, and a secondary electron-generating material
234 is coated on a bottom surface of the metal gate substrate 232. [49] Like the structure of FIG. 3a, some electron beams 301, i.e., the flow of electrons emitted from a field emitter 214, pass through the opening 236 without collision with the metal gate substrate 232, and the other electron beams collide with the secondary electron-generating material 234 coated on the metal gate substrate 232 and generate secondary electrons e. [50] Compared to the structure of FIG. 3a, an area of a side surface of the metal gate substrate 232 on which the secondary electron-generating material 234 is coated is larger, so that more secondary electrons e can be generated. [51] If necessary, the secondary electron-generating material 234 may be coated only on a side surface of the metal gate substrate 232 adjacent to the opening 236, or only on a bottom surface of the metal gate substrate 232. [52] Here, to prevent accumulation of charges in the secondary electron-generating materials 234 as described above, the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 4b. [53] Alternatively, the secondary electron-generating material 234 may be coated on bottom and top surfaces of the gate substrate 232, and the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 4c. [54] A width of the filed emitter 214 may be formed larger than a diameter of the opening
236 to generate more secondary electrons e, which is not dependant on a location of the secondary electron-generating material 234. [55] FIG. 5 illustrates generation of secondary electrons in a metal gate substrate having an opening with a tapered longitudinal- section according to still another exemplary embodiment of the present invention.
[56] Referring to FIG. 5a, an opening 236 with a tapered longitudinal-section may be formed in a metal gate substrate 232, and a secondary electron-generating material 234 may be coated on a bottom surface of the metal gate substrate 232, and a side surface of the metal gate substrate 232 adjacent to the opening 236.
[57] Like other exemplary embodiments, some electron beams 301, i.e., the flow of electrons emitted from a field emitter 214, pass through the opening 236 without collision with the metal gate substrate 232, and the other electron beams collide with the secondary electron-generating material 234 coated on the metal gate substrate 232, and generate secondary electrons e.
[58] Compared to other exemplary embodiments described above, the structure of FIG. 5a can reduce a loss of electron beams which leak through the metal gate substrate 232.
[59] If necessary, the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236, or only on the bottom surface of the metal gate substrate 232.
[60] Here, to prevent accumulation of charges in the secondary electron-generating materials 234 as described above, the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 5b.
[61] Alternatively, the secondary electron-generating material 234 may be coated on the bottom and top surfaces of the metal gate substrate 232, and the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 5c.
[62] A width of the field emitter 214 may be formed larger than a diameter of the opening
236 to generate more secondary electrons e, which is not dependant on a location of the secondary electron-generating material 234.
[63] FIG. 6 illustrates generation of secondary electrons in a metal gate substrate having an opening with a longitudinal-section which has a tapered lower region, and a reverse- tapered upper region according to yet another exemplary embodiment of the present invention.
[64] Referring to FIG. 6, a metal gate substrate 232 has an opening 236 with a longitudinal-section having a tapered lower region and a reverse-tapered upper region, and a secondary electron-generating material 234 is coated on a bottom surface of the metal gate substrate 232 and a side surface thereof adjacent to the tapered lower region of the opening 236.
[65] Like other exemplary embodiments, some electron beams 301, i.e., the flow of electrons emitted from a field emitter 214 pass through an opening 236 without collision with the metal gate substrate 232, and the other electron beams collide with the secondary electron-generating material 234 coated on the metal gate substrate 232 and generate secondary electrons e.
[66] The structure of FIG. 6a described above can reduce a loss of electron beams which leak through the metal gate substrate 232, like the structure of FIG. 5a. In addition, the structure of FIG. 6a facilitates the flow of the generated electrons e to an anode, compared to the structure of FIG. 5a.
[67] If necessary, the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236, or only on the bottom surface of the metal gate substrate 232.
[68] Here, to prevent accumulation of charges on the secondary electron-generating material 234 as described above, the secondary electron-generating material 234 may be coated only on the side surface of the metal gate substrate 232 adjacent to the opening 236, which is illustrated in FIG. 6b.
[69] Alternatively, the secondary electron-generating material 234 may be coated on the bottom and top surfaces of the metal gate substrate 232, and the side surface thereof adjacent to the opening 236, which is illustrated in FIG. 6c.
[70] A width of the field emitter 214 may be formed larger than a diameter of the opening
236 to generate more secondary electrons e, which is not dependent on a location of the secondary electron-generating material 234.
[71] While the invention has been shown and described with reference to certain exemplary embodiments thereof, it will be understood by those skilled in the art that various changes in form and details may be made therein without departing from the spirit and scope of the invention as defined by the appended claims.
Claims
[1] A field emission-back light unit, comprising: an upper substrate and a lower substrate, which are spaced apart from and face each other; an anode electrode and a phosphor layer, which are formed on the upper substrate; a cathode electrode formed on the lower substrate; a plurality of field emitters formed on the cathode electrode and spaced apart from one another; and a metal gate substrate disposed between the upper substrate and the lower substrate to induce electron emission from the field emitter, and having an opening through which the emitted electron passes, wherein at least one surface of the metal gate substrate is coated with a secondary electron-generating material capable of generating secondary electrons by collision of the emitted electrons.
[2] The field emission-back light unit according to claim 1, wherein the opening is formed in a location corresponding to each field emitter.
[3] The field emission-back light unit according to claim 1, wherein the secondary electron-generating material is coated only on a side surface of the metal gate substrate adjacent to the opening.
[4] The field emission-back light unit according to claim 1, wherein the secondary electron-generating material is coated on a side surface of the metal gate substrate adjacent to the opening, and a bottom surface of the metal gate substrate.
[5] The field emission-back light unit according to claim 1, wherein the secondary electron-generating material is coated on a side surface of the metal gate substrate adjacent to the opening, and top and bottom surfaces of the metal gate substrate.
[6] The field emission-back light unit according to claim 1, wherein the opening has a rectangular, tapered or reverse-tapered longitudinal-section, or a longitudinal- section having a reverse-tapered upper region and a tapered lower region.
[7] The field emission-back light unit according to claim 1, wherein the secondary electron-generating material is MgO.
[8] The field emission-back light unit according to claim 1, further comprising: spacers formed between the upper substrate and the metal gate substrate, and between the lower substrate and the metal gate substrate.
[9] The field emission-back light unit according to claim 1, wherein the field emitter
is formed of any one of a carbon nano tube, a carbon nano fiber and a carbon- based synthetic material.
[10] The field emission-back light unit according to claim 1, wherein the field emitter has a width larger than a maximum diameter of the opening.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
KR1020070132748A KR20090065266A (en) | 2007-12-17 | 2007-12-17 | Field emission type back light unit |
KR10-2007-0132748 | 2007-12-17 |
Publications (1)
Publication Number | Publication Date |
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WO2009078522A1 true WO2009078522A1 (en) | 2009-06-25 |
Family
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Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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PCT/KR2008/003932 WO2009078522A1 (en) | 2007-12-17 | 2008-07-03 | Field emission type back light unit |
Country Status (2)
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KR (1) | KR20090065266A (en) |
WO (1) | WO2009078522A1 (en) |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR20010077687A (en) * | 2000-02-07 | 2001-08-20 | 김순택 | Field emission display using secondary electron amplification structure |
KR20020018266A (en) * | 2000-09-01 | 2002-03-08 | 김순택 | A field emission display |
JP2005190790A (en) * | 2003-12-25 | 2005-07-14 | Toshiba Corp | Flat type image display device |
JP2005197048A (en) * | 2004-01-06 | 2005-07-21 | Toshiba Corp | Image display device and its manufacturing method |
-
2007
- 2007-12-17 KR KR1020070132748A patent/KR20090065266A/en not_active Application Discontinuation
-
2008
- 2008-07-03 WO PCT/KR2008/003932 patent/WO2009078522A1/en active Application Filing
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR20010077687A (en) * | 2000-02-07 | 2001-08-20 | 김순택 | Field emission display using secondary electron amplification structure |
KR20020018266A (en) * | 2000-09-01 | 2002-03-08 | 김순택 | A field emission display |
JP2005190790A (en) * | 2003-12-25 | 2005-07-14 | Toshiba Corp | Flat type image display device |
JP2005197048A (en) * | 2004-01-06 | 2005-07-21 | Toshiba Corp | Image display device and its manufacturing method |
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