Photodetector

The photodetector design addresses crosstalk and electron collection efficiency issues by using a flat faceplate and specific voltage-distance relationships, ensuring minimal crosstalk and high electron collection efficiency.

JP2025120963AActive Publication Date: 2025-08-18HAMAMATSU PHOTONICS KK
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Patent Information

Application Number
JP2025100187
Authority / Receiving Office
JP · JP
Patent Type
Applications
Current Assignee / Owner
Filing Date
2025-06-16
Publication Date
2025-08-18
Estimated Expiration
2043-09-07

AI Technical Summary

Technical Problem

Existing photodetectors face challenges in suppressing crosstalk between channels, particularly when detecting multiple wavelength components, due to the spread of electron trajectories, which affects electron collection efficiency.

Method used

A photodetector design with a flat faceplate and semiconductor element configuration that satisfies specific voltage and distance relationships, including a first portion with spaced channels and optional thicker second portions, to suppress crosstalk and maintain electron collection efficiency.

Benefits of technology

The design effectively suppresses crosstalk between channels while ensuring high electron collection efficiency, particularly at the outermost channels, by setting appropriate inter-channel spacing and voltage conditions.

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Abstract

To provide a photodetector capable of reducing the crosstalk between channels.SOLUTION: A photodetector 1 comprises: a tabular incident surface plate 2 on which a photoelectric surface 2s for emitting photoelectrons in accordance with incident light is formed; and a semiconductor element 10 for detecting the photoelectrons emitted from the photoelectric surface 2s, the semiconductor element being disposed to face the photoelectric surface 2s. The semiconductor element 10 has a first portion 11 having an electron incident surface 11s facing the photoelectric surface 2s, the electron incident surface including a plurality of channels ch that are arranged separated from each other. A distance b between the photoelectric surface 2s and the electron incident surface 11s, an interval Δch between the channels ch, and a voltage V applied between the photoelectric surface 2s and the electron incident surface 11s satisfy the formula (1): distance b [mm] / interval Δch [mm]<14.4×voltage V [kV]+60.SELECTED DRAWING: Figure 3
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Description

[Technical Field]

[0001] The present disclosure relates to photodetectors. [Background technology]

[0002] Patent Document 1 describes an electron tube. This electron tube includes an input faceplate provided on one side of a side tube and having a photocathode that emits electrons in response to incident light, a stem provided on the other side of the side tube and defining a vacuum region together with the input faceplate, and a semiconductor element fixed to the vacuum side of the stem and having an electron incident portion that allows electrons emitted from the photocathode to be incident. The semiconductor element is configured as a back-illuminated semiconductor element with its front surface facing the stem and its back surface facing the input faceplate, and with the electron incident portion formed as a thin plate relative to a peripheral portion located on the outer periphery of the electron incident portion. [Prior art documents] [Patent documents]

[0003] [Patent Document 1] Japanese Patent Application Publication No. 11-040086 Summary of the Invention [Problem to be solved by the invention]

[0004] Currently, in photodetectors such as the electron tube described in Patent Document 1, there is a demand for configuring an electron incident section including multiple channels in a semiconductor element in order to detect multiple wavelength components dispersed by a spectrometer, for example. However, because the trajectory of electrons traveling from the photocathode toward the electron incident section has a certain degree of spread, a configuration is required to suppress crosstalk between channels.

[0005] An object of the present disclosure is to provide a photodetector capable of suppressing crosstalk between channels. [Means for solving the problem]

[0006] The photodetector according to the present disclosure is [1] "a photodetector comprising: a faceplate having a photocathode formed thereon that emits photoelectrons in response to incident light; and a semiconductor element arranged opposite the photocathode along a first direction for detecting the photoelectrons emitted from the photocathode, wherein the semiconductor element has a first portion having an electron incident surface that faces the photocathode and includes a plurality of channels arranged at a distance from each other along a second direction intersecting the first direction; the faceplate is flat, and satisfies the following formula (1), where b is the distance between the photocathode and the electron incident surface in the first direction, Δch is the spacing between the channels in the second direction, and V is the voltage applied between the photocathode and the electron incident surface." Distance b [mm] / Spacing Δch [mm] < 14.4 × Voltage V [kV] + 60…(1)

[0007] In this photodetector, a semiconductor element for detecting photoelectrons emitted from the photocathode has a first portion having an electron incident surface including a plurality of channels arranged at a distance from one another. This photodetector satisfies the above formula (1) when the distance between the photocathode and the electron incident surface is distance b, the channel spacing in the channel arrangement direction (second direction) is distance Δch, and the voltage applied between the photocathode and the electron incident surface is voltage V. This suppresses crosstalk between channels by appropriately setting the inter-channel spacing Δch in accordance with the voltage V between the photocathode and the electron incident surface and the expansion of the electron trajectory depending on the distance b from the photocathode to the electron incident surface. In particular, this photodetector has a flat faceplate, which makes it easy to manufacture and set the distance b between the photocathode and the electron incident surface so as to satisfy the formulas.

[0008] In a photodetector such as the electron tube described in Patent Document 1, if a semiconductor element has a relatively thick portion (the peripheral portion) formed around the electron incident portion, distortion may occur in the equipotential surface between the photocathode and the electron incident portion from the electron incident portion to the peripheral portion. In this case, the electron collection efficiency of channels in the region where the equipotential surface is distorted (e.g., channels near the peripheral portion) may be lower than the electron collection efficiency of channels in the region where the equipotential surface is not distorted (e.g., channels other than those near the peripheral portion). Therefore, even if distortion of the equipotential surface occurs near the peripheral portion, it is desirable to suppress the decrease in electron collection efficiency of channels located on the peripheral portion side.

[0009] Therefore, the photodetector according to the present disclosure may be [2] "the photodetector described in [1] above, wherein the semiconductor element has a second portion provided on at least both ends of the electron incident surface in the second direction, and formed thicker than the first portion by protruding further than the electron incident surface toward the photocathode, and the distance from the end of the electron incident surface on one side in the second direction to the end of the second portion is defined as distance e, and the distance from the end of the outermost channel on one side in the second direction to the start of the second portion satisfies the following formula (2) or the following formula (3)." Distance b[mm] / 4<distance e[mm]<distance b[mm]…(2) Distance b [mm] < distance e [mm] and distance w [mm] > 0.2 [mm]…(3)

[0010] In this photodetector, the semiconductor elements are provided on both ends of the electron incident surface in at least the channel arrangement direction, and have second portions that protrude further toward the photocathode than the electron incident surface and are formed thicker than the first portions. When the distance from the end of the electron incident surface to the end of the second portion is defined as e and the distance from the end of the outermost channel to the start of the second portion is defined as w, this photodetector satisfies formula (2) or formula (3) above. This prevents a decrease in electron collection efficiency in the outermost channel even if distortion occurs from the electron incident surface to the second portion with respect to the equipotential surface between the photocathode and the electron incident portion.

[0011] The photodetector according to the present disclosure may be [3] "the photodetector according to the above [1] or [2], which satisfies the following formula (4)." In this case, crosstalk between channels can be reliably suppressed. Distance b [mm] / Spacing Δch [mm] < 13.2 × Voltage V [kV] + 55…(4)

[0012] The photodetector according to the present disclosure may be [4] "the photodetector according to the above [3], which satisfies the following formula (5)." In this case, crosstalk between channels can be more reliably suppressed. Distance b [mm] / Spacing Δch [mm] < 12.4 × Voltage V [kV] + 51.5…(5)

[0013] The photodetector according to the present disclosure may be [5] "the photodetector according to the above [4], which satisfies the following formula (6)." In this case, crosstalk between channels can be more reliably suppressed. Distance b [mm] / Spacing Δch [mm] < 12 × Voltage V [kV] + 50…(6)

[0014] The photodetector according to the present disclosure may be [6] "the photodetector according to any one of the above [1] to [5], comprising: a side tube one end of which is sealed by the faceplate; a stem sealing the other end of the side tube; and an insulating base member provided on the stem, wherein the semiconductor element is provided on the base member so that the electron incident surface faces the photocathode." In this case, by setting the dimensions of the side tube, faceplate, and base member, it is possible to achieve, for example, the distance b that satisfies the above formula.

[0015] The photodetector according to the present disclosure may be [7] "the photodetector according to any one of the above [1] to [6], which comprises an insulating film having a thickness of 100 nm or less, provided on at least a surface of the semiconductor element facing the photocathode." In this case, the insulating film formed on at least the surface of the semiconductor element prevents ionized gas generated by photoelectrons being bombarded into the semiconductor element from returning to the photocathode (ion feedback). [Effects of the Invention]

[0016] According to the present disclosure, it is possible to provide a photodetector capable of suppressing crosstalk between channels. [Brief explanation of the drawings]

[0017] [Figure 1] 1 is a schematic cross-sectional view of a photodetector according to an embodiment of the present invention. [Figure 2] FIG. 2 is a top view showing a portion of the photodetector shown in FIG. 1. [Figure 3] FIG. 2 is an enlarged view of a portion of the photodetector shown in FIG. [Figure 4] FIG. 3 is a partially enlarged view of the semiconductor element shown in FIG. 2. [Figure 5] 10 is a graph showing the relationship between voltage V and distance b when crosstalk between channels is 0%, for each value of the channel spacing Δch. [Figure 6] 10 is a graph showing the relationship between voltage V and distance b for each value of crosstalk when the channel spacing Δch is 50 μm. [Figure 7] 10 is a graph showing the relationship between voltage V and distance b for each value of crosstalk when the channel spacing Δch is 100 μm. [Figure 8] FIG. 8 is a graph showing the relationship between the distance b normalized by the distance e and the collection efficiency of the outermost channel for each distance e. [Figure 9] 10 is a graph showing the relationship between distance e and collection efficiency for each value of distance w when distance e is greater than distance b. DETAILED DESCRIPTION OF THE INVENTION

[0018] A photodetector according to one embodiment will be described below with reference to the drawings. In the description of the drawings, identical or corresponding elements are denoted by the same reference numerals, and redundant description may be omitted. Each drawing may also show a Cartesian coordinate system consisting of an axis defining a first direction D1, an axis defining a second direction D2 intersecting the first direction D1, and an axis defining a third direction intersecting the first direction D1 and the second direction D2.

[0019] Fig. 1 is a schematic cross-sectional view of a photodetector according to this embodiment. Fig. 2 is a top view showing a part of the photodetector shown in Fig. 1. Hatching is omitted in Fig. 1. The photodetector 1 shown in Figs. 1 and 2 is, for example, a HPD (hybrid photodetector), and can be used, for example, in a fluorescence microscope, a flow cytometer, a time-resolved measurement device, etc.

[0020] The photodetector 1 includes a faceplate 2, a photocathode 2s, a side tube 3, a stem 4, a base member 5, pins 6, an insulating film 7, and a semiconductor element 10. The faceplate 2 includes a front surface 2a and a back surface 2b opposite the front surface 2a. It is made of an optically transparent material such as glass, and transmits light incident on the front surface 2a toward the back surface 2b. The faceplate 2 is formed, for example, in the shape of a circular flat plate (i.e., disk). The faceplate 2 being flat means that, for example, the thickness of a relatively thick portion of the faceplate 2 in the direction from the front surface 2a to the back surface 2b (first direction D1) is within a range of approximately 130% of the thickness of a relatively thin portion.

[0021] The photocathode 2s is provided on the back surface 2b of the faceplate 2. The photocathode 2s includes a photoelectric conversion layer made of a thin film of a compound semiconductor such as GaAs, and emits photoelectrons in response to incident light that has passed through the faceplate 2.

[0022] The side tube 3 is made of an insulating material such as ceramic and has a tubular (circular) shape with both ends open. One end of the side tube 3 is sealed by the faceplate 2. The stem 4 is made of an insulating material such as ceramic and has a plate-like (disk-like) shape, and seals the other end of the side tube 3. This creates a vacuum region within the side tube 3. Metal members, made of Kovar or the like, which also serve as connecting members, are interposed between one end of the side tube 3 and the faceplate 2, and between the other end of the side tube 3 and the stem 4. A voltage can be applied to both ends via these metal members, for example, so that the stem 4 side is at GND potential relative to the photocathode 2s (so that the photocathode 2s is at a negative potential and the stem 4 side is at ground potential).

[0023] The base member 5 is provided on the stem 4 so as to be positioned within the side tube 3. The base member 5 has a top surface 5a that faces the photocathode 2s, and is formed in the shape of a rectangular parallelepiped block made of an insulating material such as ceramic, protruding convexly from the stem 4 toward the photocathode 2s. A plurality of pins 6 (for example, the same number as the channels ch described below) penetrate the base member 5 so that each pin can output an electrical signal detected by the semiconductor element 10 to the outside. For example, one end of each pin 6 reaches the surface of the base member 5 opposite the stem 4 (top surface 5a), and the other end of each pin 6 protrudes from the surface of the base member 5 facing the stem 4 to the outside of the side tube 3. The base member 5 may be formed integrally with the stem 4, or the pins 6 and the semiconductor element 10 may be electrically connected via other conductive members such as wiring.

[0024] The semiconductor element 10 is for detecting photoelectrons emitted from the photocathode 2s. The semiconductor element 10 is disposed on the top surface 5a of the base member 5 so as to face the photocathode 2s along the first direction D1. More specifically, the semiconductor element 10 includes a back surface 10r and a front surface 10s, and is provided on the top surface 5a of the base member 5 so that the back surface 10r (i.e., an electron incident surface 11s, described later) faces the photocathode 2s (so that the front surface 10s faces the top surface 5a of the base member 5). The semiconductor element 10 is electrically connected to the pins 6 by, for example, a bump connection. The semiconductor element 10 is, for example, an avalanche diode (AD). In this case, the semiconductor element 10 receives photoelectrons from the photocathode 2s, causing multiplication by electron bombardment and further multiplication by avalanche multiplication. The semiconductor element 10 may be a PD (Photo diode), SiPM (Silicon photomultiplier), or SPAD (Single photon avalanche diode). In this embodiment, the semiconductor element 10 is a back-illuminated semiconductor element.

[0025] The semiconductor device 10 has a first portion 11 and a second portion 12. The first portion 11 has an electron incident surface 11s that faces the photocathode 2s. The electron incident surface 11s includes multiple channels ch that are spaced apart and arranged along a second direction D2 that intersects with the first direction D1. In other words, the electron incident surface 11s is a photoelectron detection surface of the semiconductor device 10 and includes a sensitive region that is a multiple number of channels ch and an insensitive region surrounding each individual channel ch. The insensitive region includes a partition between adjacent channels ch (a region corresponding to the region indicated by the distance Δch described below) and a region provided between the outermost channel ch and the second portion 12 described below (a region corresponding to the region indicated by the distance w described below). The semiconductor device 10 detects photoelectrons in each of the multiple channels ch. The second portion 12 is provided at least on both ends of the electron incident surface 11s in the second direction D2. In this embodiment, the second portion 12 is formed in a rectangular frame shape surrounding the electron incident surface 11s when viewed from the first direction D1. The second portion 12 protrudes further toward the photocathode 2s than the electron incident surface 11s, and is thereby formed thicker than the first portion 11. A potential is applied between the photocathode 2s and the electron incident surface 11s so that photoelectrons emitted from the photocathode 2s move toward the electron incident surface 11s with a desired acceleration, and in this embodiment, a voltage is applied so that the electron incident surface 11s side is at GND potential (so that the photocathode 2s is at a negative potential and the electron incident surface 11s side is at ground potential).

[0026] The insulating film 7 is provided on at least the surface of the semiconductor element 10 facing the photocathode 2s. In this embodiment, the insulating film 7 is formed on the surfaces of the semiconductor element 10, the base member 5, the stem 4, and the pins 6. The insulating film 7 is preferably formed of, for example, a metal oxide (e.g., aluminum oxide) to a thickness of approximately 100 nm or less, and in this embodiment, it is formed to a thickness of approximately 30 nm or less. This prevents the insulating film 7 from affecting the incidence of photoelectrons on the electron incident surface 11s or the electrical connection of the pins 6. The insulating film 7 can be formed, for example, by performing atomic layer deposition (ALD) on a unit consisting of the semiconductor element 10, the base member 5, the stem 4, and the pins 6.

[0027] Next, the relationship between the various parts of the photodetector 1 will be described. Fig. 3 is a partially enlarged view of the photodetector shown in Fig. 1. Fig. 4 is a partially enlarged view of the semiconductor element shown in Fig. 2. Fig. 4(a) is an enlarged perspective view of region A1 in Fig. 2, and Fig. 4(b) is a schematic enlarged cross-sectional view of region A2 in Fig. 2. Fig. 4(b) also shows an equipotential surface Sv corresponding to the voltage applied between the photocathode 2s and the electron incident surface 11s.

[0028] 3 and 4, in the following description, the distance between the photocathode 2s and the electron incident surface 11s in the first direction D1 is referred to as distance b, and the spacing between the channels ch in the second direction D2 is referred to as spacing Δch. Furthermore, the voltage applied between the photocathode 2s and the electron incident surface 11s is referred to as voltage V, the distance from the end of the electron incident surface 11s on one side in the second direction D2 (the end on one side in the second direction D2) to the end of the second portion 12 (the end on one side in the second direction D2) is referred to as distance e, and the distance from the end of the outermost (edgemost) channel ch on one side in the second direction D2 (the end on the electron incident surface 11s side) to the start of the second portion 12 (the end of the first portion 11 located on one side in the second direction D2) is referred to as distance w.

[0029] The distance w is the distance from the end of the outermost channel ch (the end on one side in the second direction D2) to the rising portion of the second portion 12. Furthermore, if a member (e.g., wiring, etc.) having the same potential (or approximately the same potential) as the electron incident surface 11s is provided further outward than the end of the second portion 12, the distance e may be the distance to the end of that member. Furthermore, the distances e and w may be set similarly on the other side in the second direction D2, or may be set similarly in the third direction D3 when the channels ch are arranged along the third direction D3. Furthermore, the channel ch is an electron collector that is a semiconductor region inside the semiconductor element 10, and the interval Δch is the interval between the electron collectors. If guard rings that are separate semiconductor regions are formed around the edges of the electron collectors, the interval Δch may be the distance between the guard rings.

[0030] In the photodetector 1, the distance b, voltage V, distance e, and distance w set as described above satisfy a certain relationship from the viewpoint of suppressing crosstalk between channels ch and suppressing a decrease in the electron collection efficiency of the outermost channel ch.

[0031] FIG. 5 is a graph showing the relationship between voltage V and distance b for each value of the channel spacing Δch when crosstalk between channels is 0%. FIG. 6 is a graph showing the relationship between voltage V and distance b for each value of crosstalk when the channel spacing Δch is 50 μm. Furthermore, FIG. 7 is a graph showing the relationship between voltage V and distance b for each value of crosstalk when the channel spacing Δch is 100 μm. Note that crosstalk between channels ch means that photoelectrons emitted from a region of photocathode 2s facing one channel ch in the first direction D1 are incident on another channel ch adjacent to the one channel ch.

[0032] As shown in FIG. 5, it was found that when suppressing crosstalk between channels ch to 0%, there is a certain relationship between voltage V and distance b for each interval Δch. Furthermore, as shown in FIGS. 6 and 7, the relationship between voltage V and distance b shown in FIG. 5 tends to be similar even when the allowable crosstalk is set to values between 0% and 20%. Therefore, in the photodetector 1, when suppressing crosstalk to about 20%, the following formula (1) is satisfied. In other words, in the photodetector 1, by satisfying the following formula (1), crosstalk between channels ch can be suppressed to about 20%. Distance b [mm] / Spacing Δch [mm] < 14.4 × Voltage V [kV] + 60…(1)

[0033] On the other hand, Fig. 8 is a graph showing the relationship between the distance b normalized by the distance e and the collection efficiency of the outermost channel for each distance e. As shown in Fig. 8, even when the distance e is 1 [mm], which is the strictest condition for collection efficiency, it was confirmed that a collection efficiency of 80% or more can be obtained when the distance b is in the range of approximately 1 [mm] to 4 [mm]. Therefore, in the photodetector 1, when the collection efficiency of electrons in the outermost channel ch is set to 80% or more and the distance e is smaller than the distance b, the following formula (2) is satisfied. In other words, in the photodetector 1, by satisfying the following formula (2), the collection efficiency of electrons in the outermost channel ch is ensured to be 80% or more. Distance b[mm] / 4<distance e[mm]<distance b[mm]…(2)

[0034] On the other hand, Fig. 9 is a graph showing the relationship between distance e and collection efficiency for each value of distance w when distance e is greater than distance b. Fig. 9 illustrates the cases where distance W = 0 [mm], 0.2 [mm], 0.4 [mm], 0.5 [mm], 0.6 [mm], 0.8 [mm], and 1 [mm]. As shown in Fig. 9, in the photodetector 1, when distance e is greater than distance b, and distance w is 0.2 [mm] or greater, a collection efficiency of 95% or greater is obtained for each distance e. Therefore, in the photodetector 1, by satisfying the following formula (3), a decrease in electron collection efficiency is suppressed. Distance b [mm] < distance e [mm] and distance w [mm] > 0.2 [mm]…(3)

[0035] The above formula (1) is required to suppress crosstalk between channels ch to about 20%. Therefore, in order to further suppress crosstalk between channels ch in the photodetector 1, the following formulas (4) to (6) can be satisfied. In the photodetector 1, by satisfying the following formula (4), crosstalk can be suppressed to about 10%, by satisfying the following formula (5), crosstalk can be suppressed to about 3%, and by satisfying the following formula (6), crosstalk can be suppressed to about 0%. Distance b [mm] / Spacing Δch [mm] < 13.2 × Voltage V [kV] + 55…(4) Distance b [mm] / Spacing Δch [mm] < 12.4 × Voltage V [kV] + 51.5…(5) Distance b [mm] / Spacing Δch [mm] < 12 × Voltage V [kV] + 50…(6)

[0036] The distance b can be, for example, 0 mm to 20 mm. The distance b is preferably 0.5 mm to 10 mm, and more preferably 1 mm to 6 mm. The voltage V can be, for example, 0.1 kV to 8 kV. The voltage V is preferably 1 kV to 7 kV, and more preferably 2 kV to 6 kV. The gap Δch can be, for example, 0.01 mm to 0.5 mm. The gap Δch is preferably 0.01 mm to 0.3 mm, and more preferably 0.03 mm to 0.2 mm.

[0037] The distance e can be set to 0.1 mm to 10 mm, for example. The distance e is preferably set to 1 mm to 5 mm, and more preferably set to 1 mm to 3 mm. The distance w can be set to 0 mm to 10 mm, for example. The distance w is preferably set to 0 mm to 1 mm, and more preferably set to 0 mm to 0.3 mm. The crosstalk can be set to about 20%, preferably about 10%, and more preferably about 3% or 0%.

[0038] As described above, in the photodetector 1 according to this embodiment, the semiconductor element 10 for detecting photoelectrons emitted from the photocathode 2s has a first portion 11 having an electron incident surface 11s including a plurality of channels ch arranged at a distance from one another. In the photodetector 1, the distance b between the photocathode 2s and the electron incident surface 11s, the spacing Δch between the channels ch in the arrangement direction of the channels ch (second direction), and the voltage V applied between the photocathode 2s and the electron incident surface 11s satisfy the above formula (1). This suppresses crosstalk between the channels ch by appropriately setting the spacing Δch between the channels ch in accordance with the voltage V between the photocathode 2s and the electron incident surface 11s and the expansion of the electron trajectory depending on the distance b from the photocathode 2s to the electron incident surface 11s. In particular, the photodetector 1 has a flat faceplate 2, which facilitates fabrication and facilitates setting the distance b between the photocathode 2s and the electron incident surface 11s to satisfy the formulas. Furthermore, if the faceplate 2 is not flat, it is possible to adjust the distance b by, for example, protruding the area where the photocathode 2s is formed toward the semiconductor element 10 (for example, by making only the area where the photocathode 2s is formed thick and convex). In this case, the thickness of the faceplate 2 increases the possibility that the incident light itself will crosstalk within the faceplate 2. For this reason, it is preferable that the faceplate 2 be flat and have a thickness that allows it to maintain mechanical strength (for example, 1 mm or more).

[0039] Furthermore, in the photodetector 1, the semiconductor element 10 is provided on both ends of the electron incident surface 11s at least in the arrangement direction of the channels ch, and has second portions 12 that protrude further toward the photocathode 2s than the electron incident surface 11s, thereby being thicker than the first portions 11. In the photodetector 1, the distance e from the end of the electron incident surface 11s to the end of the second portions 12 and the distance w from the end of the outermost channel ch to the beginning of the second portion 12 satisfy the above formula (2) or (3). As a result, even if distortion occurs from the electron incident surface 11s to the second portion 12 with respect to the equipotential surface Sv between the photocathode 2s and the electron incident surface 11s, a decrease in the electron collection efficiency in the outermost channel ch is suppressed. As described above, the photodetector 1 can suppress crosstalk between channels ch and a decrease in electron collection efficiency.

[0040] Furthermore, the photodetector 1 can satisfy the above formulas (4) to (6), which makes it possible to reliably suppress crosstalk between channels.

[0041] The photodetector 1 also includes a side tube 3, one end of which is sealed by a faceplate 2, a stem 4 that seals the other end of the side tube 3, and an insulating base member 5 that is provided on the stem 4. The semiconductor element 10 is provided on the base member 5 so that the electron incident surface 11s faces the photocathode 2s. Therefore, by setting the dimensions of the side tube 3, faceplate 2, and base member 5, it is possible to achieve a distance b that satisfies the above formula, for example.

[0042] Furthermore, the photodetector 1 includes an insulating film 7 having a thickness of 100 nm or less, which is provided on at least the surface of the semiconductor element 10 facing the photocathode 2s. Therefore, the insulating film 7 formed on at least the surface of the semiconductor element 10 prevents ionized gas generated by photoelectrons being bombarded into the semiconductor element 10 from returning to the photocathode 2s (ion feedback).

[0043] The above embodiment has described one aspect of the photodetector according to the present invention. Therefore, the photodetector according to the present invention is not limited to the above embodiment and can be modified as desired.

[0044] For example, the photodetector 1 may not have the insulating film 7. Furthermore, when only focusing on suppressing crosstalk between channels ch, the photodetector 1 may not satisfy the above formulas (2) and (3). In this case, the semiconductor element 10 may not have the second portion 12. That is, although a back-illuminated semiconductor element is used as the semiconductor element 10 in this embodiment, a front-illuminated semiconductor element may also be used.

[0045] Furthermore, in this embodiment, the photocathode 2s includes a photoelectric conversion layer made of a thin film of a compound semiconductor, but the photocathode 2s may include a photoelectric conversion layer containing an alkali metal. Furthermore, in this embodiment, the base member 5 is formed into a rectangular parallelepiped block shape made of an insulating material such as ceramic and protruding from the stem 4 toward the photocathode 2s, but the base member 5 may also be a plate-like member made of an insulating material such as ceramic. In this case, the stem 4 may be provided with a fixing portion for fixing the base member 5 at a desired position. [Explanation of symbols]

[0046] 1...photodetector, 2...incident faceplate, 3...side tube, 4...stem, 5...base member, 7...insulating film, 10...semiconductor element, 11...first part, 11s...electron incident surface, 12...second part, b, e, w...distance, ch...channel, V...voltage.

Claims

1. an incident faceplate having a photocathode formed thereon that emits photoelectrons in response to incident light; a semiconductor element disposed opposite the photocathode along a first direction, the semiconductor element detecting the photoelectrons emitted from the photocathode; Equipped with the semiconductor element has a first portion having an electron incident surface facing the photocathode, the first portion including a plurality of channels arranged at intervals along a second direction intersecting the first direction; the faceplate is flat, When the distance between the photocathode and the electron incident surface in the first direction is a distance b, the spacing between the channels in the second direction is a spacing Δch, and the voltage applied between the photocathode and the electron incident surface is a voltage V, the following formula (1) is satisfied: Distance b [mm] / spacing Δch [mm] < 14.4 × voltage V [kV] + 60... (1) The distance b is 0.5 mm to 20 mm, a plurality of the channels are opposed to one of the photocathode surfaces; Photodetector.

2. Satisfies the following formula (4): Distance b [mm] / spacing Δch [mm] < 13.2 × voltage V [kV] + 55 (4) The photodetector of claim 1 .

3. Satisfies the following formula (5): Distance b [mm] / spacing Δch [mm] < 12.4 × voltage V [kV] + 51.5 ... (5) 3. The photodetector of claim 2.

4. Satisfies the following formula (6): Distance b [mm] / spacing Δch [mm] < 12 × voltage V [kV] + 50... (6) 4. The photodetector of claim 3.

5. The semiconductor element performs electron multiplication. The photodetector of claim 1 .

6. The semiconductor element is a back-illuminated type. The photodetector of claim 1 .

7. The semiconductor element is any one of an avalanche diode, a photodiode, a SiPM, and a SPAD. The photodetector of claim 1 .

8. The distance b is 0.5 mm to 10 mm. The photodetector of claim 1 .

9. The distance b is 1 mm to 6 mm.

9. The photodetector of claim 8.

10. The voltage V is 0.1 [kV] to 8 [kV]. The photodetector of claim 1 .

11. The voltage is 1 kV to 7 kV. The photodetector of claim 10.

12. The voltage is 2 [kV] to 6 [kV]. The photodetector of claim 11.

13. The interval Δch is 0.01 [mm] to 0.5 [mm]. The photodetector of claim 1 .

14. The interval Δch is 0.01 [mm] to 0.3 [mm].

14. The photodetector of claim 13.

15. The interval Δch is 0.03 [mm] to 0.2 [mm].

15. The photodetector of claim 14.

16. the semiconductor element includes a front surface and a back surface; one of the front surface and the back surface faces the photocathode, a surface facing the photocathode having the electron incident surface including a plurality of the channels; The photodetector of claim 1 .

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