JP5789223B2 - Radiation imaging apparatus and radiation imaging system - Google Patents

Description

  The present invention relates to a radiation imaging apparatus and a radiation imaging system that can be applied to a medical diagnostic imaging apparatus, a nondestructive inspection apparatus, an analysis apparatus using radiation, and the like.

  Radiation imaging apparatuses have begun to be applied widely from general imaging for acquiring still images such as X-ray imaging to fluoroscopic imaging for acquiring moving images. 2. Description of the Related Art A radiation imaging apparatus uses a sensor panel in which a plurality of pixels each having a conversion element and a switch element that convert radiation or light from a wavelength converter into electric charges are two-dimensionally arranged on a substrate. In particular, a conversion element formed of an amorphous semiconductor such as amorphous silicon (hereinafter referred to as “a-Si”) on an insulating substrate and a thin film transistor (hereinafter referred to as “TFT”) formed of an amorphous semiconductor. A flat panel detector (hereinafter referred to as “FPD”) in which a plurality of pixels are arranged two-dimensionally has attracted attention.

  Patent Document 1 discloses a PIN FPD in which a plurality of pixels including a PIN photodiode and a TFT are two-dimensionally arranged. The PIN type FPD has a laminated structure in which a layer constituting a PIN type photodiode is provided on a layer constituting a TFT on a substrate.

  Patent Document 2 discloses an MIS type FPD using a sensor panel in which a plurality of pixels each constituted by an MIS type photosensor and a TFT formed of a-Si are two-dimensionally arranged. This MIS type FPD has a planar structure in which a MIS type photosensor is provided in the same layer configuration as the layer constituting the TFT on the substrate.

  Patent Document 3 discloses a MIS type FPD having a laminated structure in which a layer constituting a MIS type photosensor is provided on a layer constituting a TFT on a substrate.

Japanese translation of Japanese translation of PCT publication No. 07-502865 JP 08-116044 A JP 2004-015002 A

SUMMARY OF THE INVENTION An object of the present invention is to allow light to efficiently enter a conversion element that converts radiation or light corresponding to the radiation into electric charges in a radiation imaging apparatus having a configuration in which light is incident from the back surface of a substrate.

According to a first aspect of the present invention, a plurality of pixels each including a conversion element that converts radiation or light corresponding to the radiation into electric charge and a switch element connected to the conversion element are arranged in a matrix. A substrate having a first surface and a second surface opposite to the first surface, and a light that is disposed on the second surface side of the substrate and is different from the radiation or the light corresponding to the radiation And a light source for irradiating the conversion element with the light source, wherein the conversion element is between the first electrode layer, the first electrode layer, and the first surface of the substrate. A second electrode layer disposed and having a gap; a semiconductor layer disposed between the first electrode layer and the second electrode layer; and between the first electrode layer and the semiconductor layer. The first impurity semiconductor layer, the second electrode layer, and the semiconductor layer Second has the impurity semiconductor layer, the light emitted from the light source, the semiconductor layer through the gap disposed between and between the semiconductor layer and the first surface of the gap Ru is incident on.

A second aspect of the present invention relates to a radiation imaging system, and includes the radiation imaging apparatus described above and a signal processing unit that processes a signal from the radiation imaging apparatus.

According to the present invention, in a radiation imaging apparatus having a configuration in which light is incident from the back surface of a substrate, light can be efficiently incident on a conversion element that converts radiation or light corresponding to the radiation into electric charges.

1 is a plan view exemplarily showing a configuration of a radiation imaging apparatus according to a preferred embodiment of the present invention. 1 is a schematic plan view of one pixel according to a preferred first embodiment of the present invention. FIG. 3 is a schematic cross-sectional view taken along line X-X ′ in FIG. 2. FIG. 3 is a schematic cross-sectional view taken along Y-Y ′ in FIG. 2. It is a typical top view of conversion element repair concerning a suitable 2nd embodiment of the present invention. It is a typical top view of 1 pixel concerning a suitable 3rd embodiment of the present invention. It is typical sectional drawing in X-X 'of FIG. It is typical sectional drawing of a radiation imaging device. It is a typical top view of 1 pixel concerning a suitable 4th embodiment of the present invention. FIG. 10 is a schematic cross-sectional view taken along line X-X ′ of FIG. 9. FIG. 10 is a schematic plan view of one pixel according to a preferred fifth embodiment of the present invention. It is typical sectional drawing in X-X 'of FIG. It is a typical top view of the 1 pixel sensor part in the laminated structure similar to the suitable 6th Embodiment of this invention. It is a typical top view of the lower electrode of a conversion element. It is a typical top view of the upper electrode of a conversion element. It is typical sectional drawing in X-X 'of FIG. It is a typical top view of 1 pixel concerning a suitable 7th embodiment of the present invention. It is typical sectional drawing in X-X 'of FIG. It is typical sectional drawing in Y-Y 'of FIG. It is a typical top view of 1 pixel concerning a suitable 8th embodiment of the present invention. It is typical sectional drawing in X-X 'of FIG. It is a typical top view of 1 pixel concerning a suitable 9th embodiment of the present invention. It is typical sectional drawing in X-X 'of FIG. It is a typical top view of 1 pixel concerning a suitable 10th embodiment of the present invention. It is typical sectional drawing in X-X 'of FIG. FIG. 14 is a schematic cross-sectional view taken along the line X-X ′ of FIG. It is a figure which shows the application example at the time of applying the radiation imaging device which concerns on suitable embodiment of this invention to a radiation imaging system.

  FIG. 1 is a plan view exemplarily showing the configuration of the radiation imaging apparatus. Reference numeral 101 denotes a conversion element that converts radiation into electric charge, 102 denotes a switching element, 103 denotes a drive wiring, 104 denotes a signal wiring, and 105 denotes a bias wiring. Reference numeral 106 denotes a signal processing circuit, 107 denotes a drive circuit, 108 denotes an A / D conversion unit, and 109 denotes a bias power supply unit. One pixel includes a conversion element 101 and a switching element 102. A plurality of pixels are two-dimensionally arranged to constitute a pixel region.

  As the insulating substrate 100, an insulating substrate such as a glass substrate, a quartz substrate, or a plastic substrate is preferably used. For example, a photoelectric conversion element is preferably used as the conversion element 101. The photoelectric conversion element is used in combination with a wavelength converter that converts radiation into light in a wavelength band that can be sensed by the photoelectric conversion element. As such a photoelectric conversion element, for example, a MIS type photoelectric conversion element and a PIN type photoelectric conversion element can be used. The MIS type photoelectric conversion element and the PIN type photoelectric conversion element are preferably formed using, for example, a-Si. Further, as the other conversion element 101, a direct type conversion element capable of directly converting radiation into electric charge may be used. Examples of such a direct conversion element include a conversion element formed using any of amorphous selenium, gallium arsenide, gallium phosphide, lead iodide, mercury iodide, CdTe, and CdZnTe. In the first to sixth embodiments, examples in which MIS type photoelectric conversion elements are applied will be described. In the seventh to eleventh embodiments, examples in which PIN type photoelectric conversion elements are applied will be described. It is not limited only to the example.

  As the switching element 102, for example, a thin film transistor (TFT) can be used. The thin film transistor (TFT) is preferably formed using a-Si.

  The drive wiring 103 is connected to the gate electrodes of the plurality of switching elements 102 arranged in the row direction, and is a wiring for applying a drive signal from the drive circuit 107 to the switching elements 102. The signal wiring 104 is connected to the source electrode or drain electrode of the plurality of switching elements 102 arranged in the column direction, and transmits the signal charges generated by the conversion element 101 and transferred by the switching element 102 to the signal processing circuit 106. belongs to. Signal charges transferred in parallel from a plurality of pixels are converted into serial signals by the signal processing circuit 106, converted from analog signals to digital signals by the A / D converter 108, and output. The bias power supply unit 109 is configured to supply a bias for the photoelectric conversion of the conversion element 101 and a bias for setting the conversion element 101 to an initial state, and a bias wiring 105 is connected to one electrode of the conversion element 101. Connected.

  Various noises can occur in the radiation imaging apparatus. Examples include shot noise, kTC noise, signal wiring noise, IC noise, gate wiring noise, and the like. Shot noise is noise proportional to the square root of the sensor aperture ratio. kTC noise is noise proportional to the square root of the capacitance of the conversion element. Signal wiring noise is wiring noise proportional to the square root of wiring resistance and wiring parasitic capacitance. IC noise is noise proportional to the parasitic capacitance of the signal wiring. The gate wiring noise is wiring noise proportional to the square root of the wiring resistance. Of these, kTC noise and signal wiring noise are dominant, and in order to reduce these noises, it is effective to reduce the capacitance of the conversion element.

  The present inventors pay attention to the fact that the capacitance of the conversion element is generally formed by the overlapping portion of the upper and lower electrodes, and ensures the output as the conversion element by considering the spread of the electric field in the portion where the upper and lower electrodes do not overlap. However, the present inventors have found a configuration in which the overlapping portion of the upper and lower electrodes of the conversion element is reduced. According to this configuration, it is possible to reduce the capacitance of the conversion element without reducing the aperture ratio of the conversion element.

Hereinafter, a radiation imaging apparatus according to a preferred embodiment of the present invention will be described in detail with reference to the drawings. In this specification, electromagnetic waves such as visible light, X-rays, α-rays, β-rays, γ-rays, and the like are also included in the radiation.
[First Embodiment]
FIG. 2 is a schematic plan view for explaining a configuration example of one pixel arranged in the radiation imaging apparatus according to the preferred first embodiment of the present invention. As shown in FIG. 2, one pixel includes a conversion element 101 and a switching element 102. The drive wiring 103 is connected to the gate electrode of the switching element 102. The signal wiring 104 is connected to the source electrode 114 a of the switching element 102. The upper electrode layer 119 of the conversion element 101 has a configuration divided into a plurality of strip-shaped electrodes 119 a, b,... Connected to the bias wiring 105. Thus, the upper electrode layer 119 has a gap 200 where the impurity semiconductor layer 118 as an ohmic contact layer does not exist.

  3 is a schematic cross-sectional view taken along line X-X ′ of FIG. 2, and FIG. 4 is a schematic cross-sectional view taken along line Y-Y ′ of FIG. 2. Hereinafter, the configuration of the pixel and the formation method thereof in this embodiment will be described in order with reference to FIGS.

  First, the gate electrode 110 of the switching element 102 and the lower electrode layer 115 of the conversion element 101 are formed on the insulating substrate 100. Next, a first insulating layer 111 to be a gate insulating film of the switching element 102 and a second insulating layer 116 to be an insulating layer of the conversion element 101 are formed. Next, a first semiconductor layer 112 serving as an active layer of the switching element 102 and a second semiconductor layer 117 serving as a conversion layer of the conversion element 101 are formed. In FIG. 3, the first semiconductor layer 112 is thinner than the second semiconductor layer 117, but the thickness may be approximately the same as that of the second semiconductor layer 117. Thereafter, a first impurity semiconductor layer 113 serving as an ohmic contact layer of the switching element 102 and a second impurity semiconductor layer 118 of the conversion element 101 are formed. Then, the bias wiring 105, the source electrode 114a and the drain electrode 114b of the switching element 102 are formed, and the first impurity semiconductor layer 113 is etched to form a channel portion. Thereafter, an upper electrode layer (transparent electrode layer) 119, a protective layer 120, and a wavelength converter (not shown) of the conversion element 101 are sequentially formed. The conversion element 101 is constituted by 115 to 119, and the switching element 102 is constituted by 110 to 114a and 114b.

  In the present embodiment, the upper electrode layer 119 has a gap 200 at least in a region where the second semiconductor layer 117 is disposed, and an electrode group 119a configured by dividing a plurality of electrodes and dispersing them in the region. , B,... The electrode groups 119a, 119,... Are electrically connected to the bias wiring 105, respectively. The width of the gap 200 may be within a range in which carriers generated by photoelectric conversion in the second semiconductor layer 117 can be captured by the expansion of the electric field from the electrode groups 119a, 119,. Although depending on the film thickness, impurity concentration, and the like of the second semiconductor layer 117, the gap 200 is preferably included in a region of 5 μm from each end of the electrode groups 119a, 119,. That is, the width of the gap 200 is preferably about 10 μm because of the spread of the electric field. The gap 200 may be formed within this range, and its shape is not particularly limited. For example, an arbitrary shape such as a polygon, a circle, an ellipse, or an indefinite shape can be taken. The configuration of the gap 200 can be similarly applied to second to eleventh embodiments described later. Since the capacitance of the conversion element 101 is generally determined by the overlapping area of the upper and lower electrodes of the conversion element 101, the conversion element of this embodiment has a structure with a reduced capacitance compared to the conventional conversion element. Noise due to the capacitance of the conversion element is reduced.

  The sensitivity of the conversion element is determined by several factors. For example, the sensitivity is determined by the amount of light incident on the semiconductor layer of the conversion element. In the radiation imaging apparatus according to this embodiment, the gap 200, that is, the region where the impurity semiconductor layer 118 of the conversion element 101 is removed and there is no useless light absorption such as light absorption that does not contribute to the output of the impurity semiconductor layer exists. Therefore, the light use efficiency of the conversion element is increased, and high sensitivity can be obtained.

Moreover, according to this embodiment, since the capacity | capacitance of a conversion element can be reduced, the size of the switch element connected to a conversion element may be small, and the aperture ratio of a conversion element can be raised. In addition, the overlapping area of the upper and lower electrodes of the conversion element is reduced, and a decrease in sensitivity can be prevented by suppressing an increase in capacitance of the conversion element accompanying an increase in the aperture ratio of the conversion element. In addition, since the size of the switch element can be small, the overlapping capacitance between the gate electrode 110 and the source electrode 114a of the switching element 102 is reduced, thereby reducing the parasitic capacitance of the signal wiring 104 and further reducing noise. Is done.
[Second Embodiment]
FIG. 5 is a schematic plan view for explaining a configuration example of one pixel arranged in the radiation imaging apparatus according to the preferred second embodiment of the present invention. In addition, the same code | symbol is attached | subjected to the component similar to 1st Embodiment. P indicates a foreign substance that causes a short circuit. R represents a region where a part of the upper electrode layer 119 and the impurity semiconductor layer 118 of the conversion element 101 is removed. The present embodiment is characterized in that when a short circuit occurs between the upper electrode layer 119 and the lower electrode layer 115 of the conversion element, the upper electrode layer 119 corresponding to the portion where the short circuit occurs is cut. As a result, a short circuit between the upper electrode layer 119 and the lower electrode layer 115 can be repaired, and a defect-free substrate can be produced at low cost. In this case, the output of the conversion element slightly decreases, but the output decrease can be compensated by output correction or the like.
[Third Embodiment]
FIG. 6 is a schematic plan view of one pixel according to the preferred third embodiment of the present invention. In addition, the same code | symbol is attached | subjected to the component similar to 1st Embodiment.

  FIG. 7 shows a schematic cross-sectional view taken along the line X-X ′ of FIG. Reference numeral 115 denotes a lower electrode layer of the conversion element 101, 116 denotes a second insulating layer that becomes an insulating layer of the conversion element 101, and 117 denotes a second semiconductor layer that becomes a photoelectric conversion layer of the conversion element 101. Reference numeral 118 denotes a second impurity semiconductor layer of the conversion element 101, and 119 denotes an upper electrode layer (transparent electrode layer) of the conversion element 101. The conversion element 101 is configured by 116 to 119. Reference numeral 120 denotes a protective layer, and a wavelength converter (not shown) is laminated on the protective layer 120.

  In this embodiment, the lower electrode layer 115 of the conversion element 101 has a comb-shaped electrode structure in which a slit 600 is formed at least in a region where the second semiconductor layer 117 is disposed. Each comb tooth has an interval of about 10 μm, and is basically connected to one of the source electrode 114 a and the drain electrode 114 b of the switching element 102 through a contact hole. Similar to the first embodiment, since the capacitance of the conversion element 101 is substantially determined by the overlapping area of the upper and lower electrodes of the sensor, the capacitance is reduced as compared with the conventional conversion element. The noise caused by is reduced. Further, the size of the switching element can be reduced by reducing the capacitance of the conversion element, and as a result, the aperture ratio of the conversion element can be further increased.

  Generally, a conversion element using amorphous silicon (hereinafter referred to as “a-Si”) is applied with a bias for a long time. Degradation of sensor characteristics may be induced. For this reason, a zero potential bias may be applied except during shooting to reduce fluctuations caused by long-term use. On the other hand, if a predetermined bias is applied only at the time of photographing, an unnecessary current is generated due to a defect in the a-Si material and the sensitivity may be lowered.

  Therefore, it is possible to reduce this phenomenon by waiting for several tens of seconds after applying a predetermined bias, but in the actual operation of the apparatus, considering immediacy, light irradiation is performed before the reading operation, and immediately, Immediate reading is possible by the driving method that enables image reading.

  FIG. 8 is a schematic cross-sectional view of the radiation imaging apparatus according to the present embodiment. Reference numeral 801 denotes a sensor substrate, 802 denotes a light source, 803 denotes a radiation source, and 804 denotes a specimen. In the sensor substrate 801, a plurality of pixels 811 are two-dimensionally arranged on an insulating substrate 810, and a wavelength converter 812 that converts the wavelength of radiation is disposed thereon. The radiation that has passed through the specimen 804 is converted into visible light 813 by the wavelength converter 812 and enters the pixel 811. On the other hand, the light source 802 has a plurality of two-dimensionally arranged LEDs 815 on the light source substrate 814 and is disposed on the back surface of the sensor substrate 801. Light 816 emitted from the light source 802 enters the pixel 811 from the back surface of the sensor substrate 801.

As described above, when light is incident from the back surface of the sensor substrate, if the structure has a gap in the lower electrode layer of the conversion element as in this embodiment, light is efficiently incident on the conversion element. It becomes possible to do. As a result, the light source can be miniaturized, and a small and lightweight device can be realized. However, since the processed shape of the lower electrode layer of the conversion element causes a short circuit between the upper and lower sides of the conversion element, highly accurate taper control is required.
[Fourth Embodiment]
FIGS. 9A and 9B are schematic plan views of one pixel according to the preferred fourth embodiment of the present invention. 9A shows the lower electrode layer side, and FIG. 9B shows the upper electrode layer side. In addition, the same code | symbol is attached | subjected to the component similar to 1st Embodiment.

  A schematic cross-sectional view taken along the line X-X ′ in FIG. 9 is shown in FIG. 10. Reference numeral 115 denotes a lower electrode layer of the conversion element 101, 116 denotes a second insulating layer that becomes an insulating layer of the conversion element 101, and 117 denotes a second semiconductor layer that becomes a photoelectric conversion layer of the conversion element 101. Reference numeral 118 denotes a second impurity semiconductor layer of the conversion element 101, and 119 denotes an upper electrode layer (transparent electrode layer) of the conversion element 101. The conversion element 101 is configured by 116 to 119. Reference numeral 120 denotes a protective layer, and a wavelength converter (not shown) is laminated on the protective layer 120.

A lower electrode layer 115 of the conversion element 101 is disposed below the region A (the gap 200) where the upper electrode layer 119 of the conversion element 101 is not disposed. On the contrary, the upper electrode layer 119 of the conversion element 101 is disposed above the region B (slit 600) where the lower electrode layer 115 of the conversion element 101 is not disposed. Further, the upper electrode layer 119 and the lower electrode layer 115 of the conversion element 101 are arranged so as to overlap with no gap. This is because when there is a gap, the electric field does not sufficiently spread, and carriers generated by photoelectric conversion do not drift smoothly. The gap between the electrodes of each conversion element 101 (the width of the gap 200 and the slit 600) is about 10 μm as in the above-described embodiment. Further, a schematic cross-sectional view taken along YY ′ in FIG. 9 is an overlapping portion of the upper and lower electrodes of the conversion element described above, and is the same as FIG. 3 of the first embodiment.
[Fifth Embodiment]
FIG. 11 is a schematic plan view of one pixel according to the preferred fifth embodiment of the present invention. In addition, the same code | symbol is attached | subjected to the component similar to 1st Embodiment.

  FIG. 12 shows a schematic cross-sectional view taken along the line X-X ′ of FIG. Reference numeral 100 denotes an insulating substrate, 110 denotes a gate electrode of the switching element 102, 111 denotes a first insulating layer that becomes a gate insulating film of the switching element 102, and 112 denotes a first semiconductor layer that becomes an active layer of the switching element 102. Reference numeral 113 denotes a first impurity semiconductor layer serving as an ohmic contact layer of the switching element 102, and 114 denotes a source electrode 114 a or a drain electrode 114 b of the switching element 102. Further, 130 is a channel protective layer of the switching element 102, 131 is a first interlayer insulating layer, and 132 is a second interlayer insulating layer.

  Reference numeral 115 denotes a lower electrode layer of the conversion element 101, 116 denotes a second insulating layer that becomes an insulating layer of the conversion element 101, and 117 denotes a second semiconductor layer that becomes a photoelectric conversion layer of the conversion element 101. Reference numeral 118 denotes a second impurity semiconductor layer of the conversion element 101, and 119 denotes an upper electrode layer (transparent electrode layer) of the conversion element 101. The conversion element 101 is configured by these 116 to 119. Reference numeral 120 denotes a protective layer, and a wavelength converter (not shown) is laminated on the protective layer 120. The upper electrode layer 119 includes an electrode 119 having a gap 200 in at least a region where the second semiconductor layer 117 is disposed.

In the present embodiment, conversion elements 101 are stacked on an array of switching elements 102 via an interlayer insulating film. The lower electrode layer 115 of the conversion element 101 is connected to the source electrode 114a or the drain electrode 114b of the switching element 102 through a contact hole, and the upper electrode layer 119 of the conversion element 101 has a gap 200 of about 10 μm square cut out. It has a shape.
[Sixth Embodiment]
FIG. 13 is a schematic plan view of a one-pixel sensor unit in a stacked structure similar to that of the preferred fifth embodiment of the present invention. FIG. 14 is a schematic plan view of the lower electrode layer of the conversion element 101, and FIG. 15 is a schematic plan view of the upper electrode layer of the conversion element 101. In the figure, the black part is an area where electrodes are present, and the superimposed state is shown in FIG. As is clear from FIG. 13, the upper electrode layer and the lower electrode layer of the conversion element 101 are arranged so as to overlap without any gap. This is because when there is a gap, the electric field does not sufficiently spread, photoelectric conversion occurs, and the generated carrier does not drift smoothly.

  FIG. 16 is a schematic cross-sectional view taken along the line X-X ′ in FIG. Reference numeral 100 denotes an insulating substrate, 110 denotes a gate electrode of the switching element 102, 111 denotes a first insulating layer that becomes a gate insulating film of the switching element 102, and 112 denotes a first semiconductor layer that becomes an active layer of the switching element 102. Reference numeral 113 denotes a first impurity semiconductor layer serving as an ohmic contact layer of the switching element 102, and 114 denotes a source electrode 114 a or a drain electrode 114 b of the switching element 102. Further, 130 is a channel protective layer of the switching element 102, 131 is a first interlayer insulating layer, and 132 is a second interlayer insulating layer.

Reference numeral 115 denotes a lower electrode layer of the conversion element 101, 116 denotes a second insulating layer that becomes an insulating layer of the conversion element 101, and 117 denotes a second semiconductor layer that becomes a photoelectric conversion layer of the conversion element 101. Reference numeral 118 denotes a second impurity semiconductor layer of the conversion element 101, and 119 denotes an upper electrode layer (transparent electrode layer) of the conversion element 101. The conversion element 101 is configured by 116 to 119. Reference numeral 120 denotes a protective layer, and a wavelength converter (not shown) is laminated on the protective layer 120.
[Seventh Embodiment]
FIG. 17 is a schematic plan view of one pixel according to the seventh preferred embodiment of the present invention. The pixel of the present application can also be applied to a radiation imaging apparatus configured as shown in FIG.

  FIG. 18 is a schematic cross-sectional view taken along the line X-X ′ of FIG. Reference numeral 215 denotes a lower electrode layer of the conversion element 201, 216 denotes a first impurity semiconductor layer of the conversion element 201, 217 denotes a second semiconductor layer serving as a photoelectric conversion layer of the conversion element 201, and 218 denotes a second impurity of the conversion element 201. A semiconductor layer 219 is an upper electrode layer (transparent electrode layer) of the conversion element 201. The conversion element 201 is a PIN photoelectric conversion element constituted by 216 to 219. Reference numeral 220 denotes a protective layer, and a wavelength converter (not shown) is laminated on the protective layer 220.

  FIG. 19 shows a schematic cross-sectional view taken along the line Y-Y ′ of FIG. Reference numeral 210 denotes a gate electrode of the switching element 202, 211 denotes a first insulating layer that becomes a gate insulating film of the switching element 202, and 212 denotes a first semiconductor layer that becomes an active layer of the switching element 202. Reference numeral 213 denotes a first impurity semiconductor layer serving as an ohmic contact layer of the switching element 202, 214 a denotes a source electrode of the switching element 202, and 214 b denotes a drain electrode of the switching element 202. Reference numeral 215 denotes a lower electrode layer of the conversion element 201 which is also the source electrode 214a or the drain electrode 214b of the switching element 202, and reference numeral 216 denotes a second insulating layer which becomes an insulating layer of the conversion element 201. Reference numeral 217 denotes a second semiconductor layer serving as a photoelectric conversion layer of the conversion element 201, 218 denotes a second impurity semiconductor layer of the conversion element 201, and 219 denotes an upper electrode layer (transparent electrode layer) of the conversion element 201. The conversion element 201 includes 216 to 219, and the bias wiring 205 and the upper electrode layer 219 are connected to form the upper electrode layer of the conversion element 201. Reference numeral 220 denotes a protective layer, and a wavelength converter (not shown) is laminated on the protective layer 220.

  In the present embodiment, the upper electrode layer 219 has a gap 200 at least in a region where the second semiconductor layer 217 is disposed, is connected to the bias wiring 205, and is an electrode group 219a composed of a plurality of strip-shaped electrodes. , B,... The electrode groups 219a, 219,... Are formed by dividing a plurality of strip-shaped electrodes and dispersing them in the region, and are electrically connected to the bias wiring 205, respectively. The second impurity semiconductor layer 218 is not present in the gap 200. The width of the opening 200 is preferably about 10 μm because of the spread of the electric field. Since the capacitance of the conversion element 201 is generally determined by the overlapping area of the upper and lower electrodes of the conversion element 201, the capacitance of the conversion element 201 is reduced compared to the conventional case. That is, noise related to the capacitance of the conversion element 201 can be reduced.

On the other hand, since the sensitivity of the conversion element 201 is substantially determined by the aperture ratio of the conversion element 201, the gap 200, that is, the second impurity semiconductor layer 218 of the sensor element is removed, and there is a region where there is no useless light absorption. Is improved. In addition, the size of the switching element 202 is reduced by reducing the capacitance of the conversion element 201, and as a result, the aperture ratio of the conversion element 201 can be further increased. As shown in FIG. 5, when a short circuit between the upper and lower sides of the conversion element 201 occurs, the upper and lower short circuit can be repaired by cutting the upper electrode layer of the corresponding conversion element 201.
[Eighth Embodiment]
FIG. 20 is a schematic plan view of one pixel according to the preferred eighth embodiment of the present invention. In addition, the same code | symbol is attached | subjected to the component similar to 7th Embodiment.

  FIG. 21 shows a schematic cross-sectional view taken along the line X-X ′ of FIG. Reference numeral 215 denotes a lower electrode layer of the conversion element 201, 216 denotes a first impurity semiconductor layer of the conversion element 201, 217 denotes a second semiconductor layer serving as a photoelectric conversion layer of the conversion element 201, and 218 denotes a second impurity of the conversion element 201. A semiconductor layer 219 is an upper electrode layer (transparent electrode layer) of the conversion element 201. The conversion element 201 includes 216 to 219. Reference numeral 220 denotes a protective layer, and a wavelength converter (not shown) is laminated on the protective layer 220.

  In the present embodiment, the lower electrode layer 215 of the conversion element 201 has a comb-shaped electrode structure in which slits 600 are formed at least in a region where the second semiconductor layer 217 is disposed. Each comb tooth has an interval of about 10 μm. Since the capacitance of the conversion element 201 is generally determined by the overlapping area of the upper and lower electrodes of the conversion element 201, the capacitance is reduced as compared with the conventional case. That is, noise related to the capacitance of the conversion element 201 can be reduced. Further, the reduction in the capacitance of the conversion element 201 can reduce the size of the switching element 202, and as a result, the aperture ratio of the conversion element 201 can be further increased.

Also in this embodiment, in the case of a conversion element using a-Si, it is possible to make light incident from the back surface of the sensor substrate as shown in FIG. 8 so that light can be efficiently incident on the conversion element. It is.
[Ninth Embodiment]
FIG. 22 is a schematic plan view of one pixel according to the ninth preferred embodiment of the present invention. 22A shows the lower electrode layer side, and FIG. 22B shows the upper electrode layer side. In addition, the same code | symbol is attached | subjected to the component similar to 7th Embodiment.

  FIG. 23 shows a schematic cross-sectional view taken along the line X-X ′ of FIG. Reference numeral 215 denotes a lower electrode layer of the conversion element 201, 216 denotes a first impurity semiconductor layer of the conversion element 201, 217 denotes a second semiconductor layer serving as a photoelectric conversion layer of the conversion element 201, and 218 denotes a second impurity of the conversion element 201. A semiconductor layer 219 is an upper electrode layer (transparent electrode layer) of the conversion element 201. The conversion element 201 includes 216 to 219. Reference numeral 220 denotes a protective layer, and a wavelength converter (not shown) is laminated on the protective layer 220.

The lower electrode layer of the conversion element 201 is disposed below the region A (the gap 200) where the upper electrode layer of the conversion element 201 is not disposed. Conversely, the upper electrode layer of the conversion element 201 is disposed above the region B (slit 600) where the lower electrode layer of the conversion element 201 is not disposed. Further, the upper electrode layer and the lower electrode of the conversion element 201 are arranged so as to overlap with no gap. This is because when there is a gap, the electric field does not sufficiently spread, photoelectric conversion occurs, and the generated carrier does not drift smoothly. The gap between the sensor electrodes is about 10 μm as in the above-described embodiment. Further, a schematic cross-sectional view taken along the line YY ′ in FIG. 22 is an overlapping portion of the upper and lower electrodes of the conversion element 201 described above, and is the same as FIG.
[Tenth embodiment]
FIG. 24 is a schematic plan view of one pixel according to the preferred tenth embodiment of the present invention. In addition, the same code | symbol is attached | subjected to the component similar to 7th Embodiment.

  FIG. 25 is a schematic cross-sectional view taken along the line X-X ′ of FIG. Reference numeral 200 denotes an insulating substrate, 210 denotes a gate electrode of the switching element 202, 211 denotes a first insulating layer which becomes a gate insulating film of the switching element 202, and 212 denotes a first semiconductor layer which becomes an active layer of the switching element 202. Reference numeral 213 denotes a first impurity semiconductor layer serving as an ohmic contact layer of the switching element 202, and 214 denotes a source electrode 214 a or a drain electrode 214 b of the switching element 202. Reference numeral 230 denotes a channel protective layer of the switching element 202, 231 denotes a first interlayer insulating layer, and 232 denotes a second interlayer insulating layer.

  Reference numeral 215 denotes a lower electrode layer of the conversion element 201, 216 denotes a first impurity semiconductor layer of the conversion element 201, and 217 denotes a second semiconductor layer that becomes a photoelectric conversion layer of the conversion element 201. Reference numeral 218 denotes a second impurity semiconductor layer of the conversion element 201, and 219 denotes an upper electrode layer (transparent electrode layer) of the conversion element 201. The conversion element 201 is a PIN photoelectric conversion element and is configured by 216 to 219. Reference numeral 220 denotes a protective layer, and a wavelength converter (not shown) is laminated on the protective layer 220. The upper electrode layer 219 includes an electrode 219 having a gap 200 in at least a region where the second semiconductor layer 217 is disposed.

In the present embodiment, the conversion element 201 is laminated on the array of switching elements 202 via a planarized interlayer insulating film. The lower electrode layer 215 is connected to the source electrode 214a or the drain electrode 214b of the switching element 202 through a contact hole, and the upper electrode layer 219 has a shape in which a gap 200 of about 10 μm square is cut out.
[Eleventh embodiment]
A schematic plan view of one pixel in the same stacked structure as that of the tenth embodiment is the same as FIG. Further, the lower electrode layer of the conversion element 101 is the same as in FIG. 14, and the upper electrode layer of the conversion element 101 is the same as in FIG.

  Also in the present embodiment, the upper electrode layer and the lower electrode layer of the conversion element 201 configured with a PIN photoelectric conversion element are arranged so as to overlap without any gap. This is because when there is a gap, the electric field does not sufficiently spread, photoelectric conversion occurs, and the generated carrier does not drift smoothly.

  FIG. 26 shows a cross-sectional view of one pixel of the tenth embodiment at the same position as the schematic cross-sectional view along X-X ′ in FIG. 13. Reference numeral 200 denotes an insulating substrate, 210 denotes a gate electrode of the switching element 202, 211 denotes a first insulating layer which becomes a gate insulating film of the switching element 202, and 212 denotes a first semiconductor layer which becomes an active layer of the switching element 202. Reference numeral 213 denotes a first impurity semiconductor layer serving as an ohmic contact layer of the switching element 202, and 214 denotes a source electrode 214 a or a drain electrode 214 b of the switching element 202. Reference numeral 230 denotes a channel protective layer of the switching element 202, 231 denotes a first interlayer insulating layer, and 232 denotes a second interlayer insulating layer.

Reference numeral 215 denotes a lower electrode of the conversion element 201, 216 denotes a first impurity semiconductor layer of the conversion element 201, 217 denotes a second semiconductor layer which becomes a photoelectric conversion layer of the conversion element 201, and 218 denotes a second impurity semiconductor of the conversion element 201. Reference numerals 219 denote upper electrode layers (transparent electrode layers) of the conversion element 201. The conversion element 201 includes 216 to 219. Reference numeral 220 denotes a protective layer, and a wavelength converter (not shown) is laminated on the protective layer 220.
[Application example]
FIG. 27 is a diagram showing an application example when the radiation imaging apparatus according to the preferred embodiment of the present invention is applied to a radiation imaging system.

  Radiation 3002 generated in the radiation tube 3001 passes through a body part 3004 such as a chest of a subject (patient or the like) 3003 and enters a radiation imaging apparatus 3000 having a scintillator (phosphor) mounted thereon. The incident radiation 3002 includes information inside the body of the subject 3003. In the radiation imaging apparatus 3000, the scintillator emits light in response to the incidence of the radiation 3002, and this is photoelectrically converted to obtain electrical information. In the radiation imaging apparatus 3000, electrical information may be obtained by directly converting the radiation 3002 into electric charges. This information is converted to digital, subjected to image processing by an image processor 3005 as signal processing means, and displayed on a display 3006 as display means in the control room.

  Further, this information can be transferred to a remote place by a transmission means 3007 such as a wireless or telephone line. As a result, it can be displayed on a display 3008 as display means installed in a doctor room or the like in another place, or can be stored in a recording medium such as an optical disk by a film processor 3009 as storage means. In this way, a remote doctor can make a diagnosis. The film processor 3009 is connected to a laser printer 3011 as a printing unit, and can record information transmitted by the transmission unit 3007 on a recording medium 3010 such as a film.

  As described above, according to the preferred embodiment of the present invention, the capacitance can be remarkably reduced without reducing the aperture ratio of the conversion element, so that kTC noise caused by the capacitance can be reduced. Furthermore, since the sensor capacity is reduced, the transfer rate can be improved. As a result, the switch element can be reduced in size, the sensor aperture ratio can be improved, the overlap capacitance between the gate and source of the switching element is reduced, the signal line parasitic capacitance is reduced, and noise Is reduced.

  In addition, there are various effects such that light incident directly on the semiconductor layer can be increased to improve the amount of incident light, or that light can be easily incident from the back surface such as light reset in moving image driving.

100 Substrate 101 Conversion element 102 Switch element 115 Second electrode layer 119 First electrode layer 119a, b, ... Electrode group 200 Gap

Claims (6)

A first surface on which a plurality of pixels each including a conversion element that converts radiation or light corresponding to the radiation into charges and a switch element connected to the conversion element are arranged in a matrix; and the first surface A substrate having a second surface opposite to the substrate;
A light source disposed on the second surface side of the substrate and for irradiating the conversion element with light different from the radiation or light according to the radiation;
A radiation imaging apparatus comprising:
The conversion element includes a first electrode layer, a second electrode layer disposed between the first electrode layer and the first surface of the substrate, and having a gap, and the first electrode layer, A semiconductor layer disposed between the second electrode layer; a first impurity semiconductor layer disposed between the first electrode layer and the semiconductor layer; the second electrode layer; A second impurity semiconductor layer disposed between the semiconductor layer and between the first surface and the semiconductor layer in the gap;
A radiation imaging apparatus, wherein light emitted from the light source is incident on the semiconductor layer through the gap. In each of the plurality of pixels, the conversion element is disposed above the switch element via an interlayer insulating film,
The switch element includes a gate electrode, a drain electrode, and a source electrode, and transfers a signal corresponding to the electric charge converted by the conversion element to a signal line, and one of the drain electrode and the source electrode is Electrically connected to the second electrode layer;
A bias wiring connected to the first electrode layer and a signal wiring connected to the other of the drain electrode and the source electrode are further disposed on the first surface of the substrate. The radiation imaging apparatus according to claim 1.   The radiation imaging apparatus according to claim 1, wherein the second electrode layer has a plurality of the gaps in a region where the semiconductor layer is disposed.   The radiation imaging apparatus according to claim 1, wherein the second electrode layer has a comb-teeth structure. The conversion element is a photoelectric conversion element,
The radiation imaging apparatus further includes a wavelength converter that converts radiation into visible light, and the substrate on which the plurality of pixels are formed on the first surface is disposed between the wavelength converter and the light source. The radiation imaging apparatus according to any one of claims 1 to 4, wherein the radiation imaging apparatus is provided. The radiation imaging apparatus according to any one of claims 1 to 5,
Signal processing means for processing signals from the radiation imaging apparatus;
A radiation imaging system comprising:

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