WO2023213872A1 - Single-photon avalanche diode - Google Patents
Single-photon avalanche diode Download PDFInfo
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- WO2023213872A1 WO2023213872A1 PCT/EP2023/061658 EP2023061658W WO2023213872A1 WO 2023213872 A1 WO2023213872 A1 WO 2023213872A1 EP 2023061658 W EP2023061658 W EP 2023061658W WO 2023213872 A1 WO2023213872 A1 WO 2023213872A1
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F77/00—Constructional details of devices covered by this subclass
- H10F77/10—Semiconductor bodies
- H10F77/14—Shape of semiconductor bodies; Shapes, relative sizes or dispositions of semiconductor regions within semiconductor bodies
- H10F77/146—Superlattices; Multiple quantum well structures
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04N—PICTORIAL COMMUNICATION, e.g. TELEVISION
- H04N25/00—Circuitry of solid-state image sensors [SSIS]; Control thereof
- H04N25/70—SSIS architectures; Circuits associated therewith
- H04N25/76—Addressed sensors, e.g. MOS or CMOS sensors
- H04N25/78—Readout circuits for addressed sensors, e.g. output amplifiers or A/D converters
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F30/00—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors
- H10F30/20—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors
- H10F30/21—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation
- H10F30/22—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation the devices having only one potential barrier, e.g. photodiodes
- H10F30/225—Individual radiation-sensitive semiconductor devices in which radiation controls the flow of current through the devices, e.g. photodetectors the devices having potential barriers, e.g. phototransistors the devices being sensitive to infrared, visible or ultraviolet radiation the devices having only one potential barrier, e.g. photodiodes the potential barrier working in avalanche mode, e.g. avalanche photodiodes
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F39/00—Integrated devices, or assemblies of multiple devices, comprising at least one element covered by group H10F30/00, e.g. radiation detectors comprising photodiode arrays
- H10F39/10—Integrated devices
- H10F39/107—Integrated devices having multiple elements covered by H10F30/00 in a repetitive configuration, e.g. radiation detectors comprising photodiode arrays
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F77/00—Constructional details of devices covered by this subclass
- H10F77/93—Interconnections
- H10F77/933—Interconnections for devices having potential barriers
Definitions
- the present disclosure is in the field of single-photon avalanche diodes (SPADs), and relates in particular to SPADs suitable for use with high excess bias voltages relative to an operating voltage of associated read-out electronics.
- SPADs single-photon avalanche diodes
- a Single Photon Avalanche Diode is a solid-state photodetector based around a semiconductor p-n junction.
- a conventional photodiode may operate with a relatively low reverse bias voltage, wherein a leakage current may change linearly with absorption of incident photons due to an internal photoelectric effect.
- a SPAD may be configured to be biased above its breakdown voltage. The reverse bias may be sufficiently high such that photons incident on the SPAD may cause impact ionization triggering generation of an avalanche current.
- a photo-generated carrier may be accelerated by an electric field in the SPAD due to the relatively high reverse bias voltage, wherein the photo-generated carrier may trigger an avalanche current due to an impact ionization mechanism.
- a SPAD may be capable of detecting incidence of individual photons.
- a SPAD biased well above its reverse-bias breakdown voltage may be known in the art as operating within a “Geiger-mode” region.
- the avalanche current may be ‘quenched’ by lowering the bias down to the breakdown voltage or lower.
- Circuits for quenching the avalanche current may be either passive, e.g. as simple as a single resistor in series with the SPAD, or active, e.g. comprising additional circuitry such as one or more transistors for actively controlling the bias voltage.
- the SPAD may be ‘reset’ in order to re-enable detection of incident photons. That is, after the avalanche breakdown is stopped, the SPAD may be recharged to its relatively high reverse bias voltage, e.g. significantly above a breakdown voltage of the SPAD.
- a SPAD or an array of SPADs may be coupled to read-out circuitry for determining whether and when the SPAD or SPADs have been triggered and/or for counting triggering events.
- a maximum usable excess bias voltage of a SPAD with integrated read-out electronics may be limited by a maximum voltage supported by low-voltage transistors used to implement the read-out circuitry.
- the maximum usable excess bias voltage of the SPAD may be limited by a maximum voltage supported by transistors or circuitry used to implement quenching.
- the integrated read-out electronics and/or quench circuit may be prone to damage.
- a high excess bias voltage may improve a performance of a SPAD.
- a high excess bias voltage may improve a Photon Detection Efficiency (PDE) and reduce jitter, resulting in an overall improved performance of a device using the SPAD.
- PDE Photon Detection Efficiency
- the present disclosure is in the field of SPADs, and relates in particular to SPADs suitable for use with high excess bias voltages relative to an operating voltage of associated read-out electronics.
- a single-photon avalanche diode comprising: a first well-region formed in a substrate; a second well-region formed on the substrate and extending at least partway around the first well-region; at least one contact formed over the second well-region; and a deep wellregion extending non-uniformly between the first well-region and the second wellregion, wherein the first well-region is formed at a junction defining an avalanche region, and wherein the second well-region and the deep well-region are configured to provide a conductive path between the avalanche region and the at least one contact.
- a single-photon avalanche diode comprising: a first well-region formed in a substrate; a second well-region formed on the substrate and extending at least partway around the first well-region; at least one contact formed over the second well-region; and a deep wellregion extending non-uniformly between the first well-region and the second wellregion, wherein the first well-region is formed at a junction
- a resistance of the conductive path between the first well-region and the at least one contact may be increased relative to a prior art SPAD where the deep well-region may extend uniformly between the first well-region and the second well-region.
- the SPAD itself is effectively implemented with an internal quenching resistor, e.g. the conductive path provides sufficient resistance to act as a quenching resistor.
- an additional external quenching resistor may also be used with the SPAD.
- an additional external quenching resistor or transistor, may also be used with the SPAD.
- a voltage seen by a transistor used for quenching may be reduced.
- the internal quenching resistor may enable the SPAD to be operated at an excess bias voltage exceeding a maximum operating voltage for low-voltage transistors that may be used to implement the read-out electronics.
- this enables the SPAD to be operated with a higher excess bias voltage, thereby improving photon detection efficiency and timing jitter, and overall product performance.
- SPADs it may sometimes be beneficial to disable one or more SPADs.
- Example reasons for this can be that some SPADs may exhibit a very high dark count rate or that in a certain application mode not all SPADs in the array are required.
- this may be implemented by connecting an anode of the SPAD to be disabled with a switch to VDD and by an additional switch in the path of the quenching transistor to avoid a permanent current flowing from VDD to VSS.
- the SPAD may not be not fully disabled but may operate with an excess bias voltage reduced by VDD. There is no problem with quenching because for small excess bias voltages the internal quenching resistor is sufficient for proper quenching. There will also be no signal detected since the input of the buffer is connected to VDD. It will be understood that extending non-uniformly may include extending with non-uniformities in a doping density and/or extending with non-uniformities in a distribution e.g. not laterally extending continuously all around the first well, as will be described in more detail below. In contrast, prior art SPADs may be implemented wherein a deep well-region may extend uniformly, e.g. with a uniform doping density between the first well-region and the second well-region and extending continuously all around the first well.
- the junction defining the avalanche region may be a pn junction.
- the pn junction may be formed between the first-well region and an implant region formed on the first well region.
- the pn junction may be formed between the first-well region and the deep well region.
- the pn junction may be formed between the first-well region and a further well region or implant region formed in the deep well region.
- the deep well-region When viewed in a direction orthogonal to a surface of the substrate, the deep well-region may extend only partway around the first well-region.
- the resistance of the conductive path between the first well-region and the at least one contact may be increased relative to a prior art SPAD wherein the deep well-region may extend uniformly between the first well-region and the second well-region.
- the deep well-region may only extend towards one or more portions of the second well, without extending below a contact formed in the second well.
- a path length of the conductive path may be relatively long, thereby increasing an overall resistance of the conductive path.
- a doping density of the deep well-region between the first well-region and the second well-region may be non-uniform.
- a doping density of the deep well-region between the first wellregion and the second well-region may be lower than a doping density of the deep wellregion directly below the first well-region and/or the second well-region.
- an overall resistance of the conductive path between the first well-region and the second wellregion may be increased.
- a region of the deep well-region between the first well-region and the second well-region may have a lower doping concentration than regions of the deep wellregion directly below the first well-region and the second well-region.
- forming the deep well region may comprise forming a first portion of the deep well-region and a second portion of the deep well-region separated by a gap, wherein a lateral spread and/or thermal diffusion of the deep well-region causes the conductive path to extend across the gap, but with a lower doping concentration within the gap.
- a size of the gap may be selected to define a resistance of the conductive path.
- the conductive path may be an indirect conductive path.
- the conductive path may not be a straight line between the first wellregion and the at least one contact.
- the deep well-region may not extend below the at least one contact
- a length of the path may be extended, because the path may have to extend along, e.g. laterally in a direction substantially parallel to a surface of the substrate, to the at least one contact.
- the second well-region and the deep well-region may not be configured to provide a direct conductive path between the avalanche region and the at least one contact.
- the conductive path may not be a straight line between the first wellregion and the at least one contact.
- the conductive path may not be the shortest path between the first well-region and the at least one contact.
- this may result in a longer path between the first well-region and the at least one contact, thereby increasing an overall resistance of the path.
- the SPAD When viewed in a cross section extending through a center of the SPAD and through the at least one contact, the SPAD may not be symmetrical.
- the deep well when viewed in the cross section, may extend only in a first direction toward the second well-region.
- the SPAD may comprise a plurality of conductive paths, each path extending in a different direction at least partway around the first well-region.
- the conductive path may extend in both directions, e.g. clockwise and anticlockwise, around the first well region.
- the SPAD may comprise an implant region formed on the first well-region to define the avalanche region of the SPAD. At least one further contact may be formed over the implant region.
- the at least one contact may provide a cathode and a conductivity type of the second well-region may be n-type, and the at least one further contact may provide an anode and the conductivity type of the implant region may be p-type.
- the at least one contact may provide an anode and a conductivity type of the second well-region may be p-type, and the at least one further contact may provide a cathode and the conductivity type of the implant region may be n-type.
- the SPAD may comprise a guard ring provided by a lightly-doped lateral region extending between the first well-region and the second well-region.
- the guard ring may extend completely around the first well-region.
- the first well-region When viewed in a direction orthogonal to a surface of the substrate, the first well-region may be disposed between the at least one contact and a location where the deep well-region extends to the second well-region.
- an array of SPADs comprising: a plurality of first well-regions formed in a substrate; a second wellregion formed on the substrate and extending at least partway around and/or between the plurality of first well-regions; at least one contact formed over the second wellregion; and a deep well-region extending non-uniformly between each first well-region and the second well-region, wherein each first well-region is formed at a junction defining a respective avalanche region, and wherein the second well-region and the deep well-region are configured to provide a conductive path between each avalanche region and the at least one contact.
- a SPAD pixel read-out circuit comprising: a SPAD according to the first aspect; and an output buffer coupled to an anode of the SPAD; wherein the SPAD is configured such that, in use, an excess bias voltage level across an avalanche region of the SPAD exceeds a voltage level at the anode and a voltage level of a power supply (VDD) the output buffer.
- VDD power supply
- a method of manufacturing a SPAD comprising: forming a deep well-region in a substrate; forming a first well-region in the deep well-region and forming a second well- region extending at least partway around the first well-region; and forming at least one contact over the second well-region, wherein the deep well-region is formed to extend non-uniformly between the first well-region and the second well-region, wherein the first well-region is formed at a junction defining an avalanche region, and wherein the second well-region and the deep well-region are formed to provide a conductive path between the avalanche region and the at least one contact.
- a resistance of the conductive path between the first well-region and the at least one contact may be increased relative to a prior art SPAD wherein the deep well-region may extend uniformly between the first well-region and the second well-region.
- Forming the deep well region may comprise forming a first portion of the deep well-region and a second portion of the deep well-region separated by a gap, wherein a lateral spread and/or thermal diffusion of the deep well-region causes the conductive path to extend across the gap.
- the first portion of the deep well-region may extend under the first well-region and the second portion of the deep well-region may extend under the second well-region.
- the deep well-region may be formed such that, when viewed in the direction orthogonal to a surface of the substrate, the deep well-region extends only partway around the first well-region such that the deep well-region does not extend below the at least one contact.
- Figure 1 depicts a schematic of a prior art SPAD pixel read-out circuit
- Figure 2 depicts a cross-sectional view and a plan view of a prior art SPAD, as may be implemented in the pixel of Figure 1 ;
- Figure 3 depicts a SPAD-based pixel according to an embodiment of the disclosure
- Figure 4 a cross-sectional view and a plan view of a SPAD according to an embodiment of the disclosure
- Figure 5 a cross-sectional view and a plan view of a SPAD according to a further embodiment of the disclosure
- Figure 6 a cross-sectional view and a plan view of a SPAD according to a further embodiment of the disclosure
- Figure 7 a cross-sectional view and a plan view of a SPAD according to a further embodiment of the disclosure.
- Figure 8a a plan view of a SPAD array according to an embodiment of the disclosure.
- Figure 8b a plan view of a SPAD array according to a further embodiment of the disclosure.
- Figure 9 depicts partial cross-sections of further configurations of SPADs, which may be combined with the concepts disclosed in Figures 4 to 8 to implement further embodiments of the disclosure.
- FIG. 1 depicts a schematic of a prior art SPAD pixel read-out circuit 100.
- the circuit 100 comprises a SPAD 105, where a cathode of the SPAD 105 is coupled to a high voltage reference VHV and an anode of the SPAD 105 is coupled to a buffer 110.
- the buffer 110 represents read-out circuitry, e.g. a circuit configured to read-out a state of the SPAD.
- the circuit 100 may be an integrated device, wherein the buffer 110 may be fabricated using low-voltage CMOS transistors.
- the buffer 110 is coupled to a supply voltage VDD.
- a voltage of the supply rail VDD is lower than a voltage of the high voltage reference VHV.
- the buffer 110 is implemented as an inverter. That is, an output of the buffer 110 represents an inverse of node C, e.g. if a voltage at node C is high, an output of the inverter is low.
- Node C corresponds to the anode of the SPAD 105
- a current mirror 115 configured to mirror a quench current IQ to the SPAD 105. That is, the current mirror 115 implements a passive quenching circuit configured to provide a constant quench current IQ. It will be understood that this is merely an example of a quenching circuit, and other quenching circuits are known in the art.
- the buffer 110 may indicate occurrence of avalanche triggering events, e.g. photon strikes, as a drop in an output voltage of the buffer 110
- a maximum usable excess bias voltage of the SPAD 105 may be limited by a maximum voltage supported by low-voltage transistors used to implement the read-out circuitry and quenching circuitry, e.g. buffer 110 and current mirror 115. If the excess bias voltage of the SPAD 105 is too high, the current mirror circuit 115 and/or the buffer 110 may be prone to damage.
- PDE Photon Detection Efficiency
- Figure 2 depicts a plan view of a prior art SPAD 200. Figure 2 also depicts a cross-sectional view of the SPAD 200 across a line A-A.
- the SPAD 200 may be implemented as the SPAD 105 in the SPAD pixel readout circuit 100 of Figure 1.
- the example SPAD 200 is formed on a P-type substrate 260.
- the example SPAD comprises a first well-region 205 formed in the substrate 260.
- the first well-region 205 is denoted an “N-enhance region”, e.g. a well heavily doped with n-type impurities.
- the second well-region 210 is an N-type well, e.g. formed by diffusion of n-type impurities into the P-type substrate 260.
- a plurality of contacts 215 are formed over the second well-region 210.
- the plurality of contacts 215 comprises an N+ diffused portion, for providing an ohmic contact to a plurality of cathodes 265, where the cathodes 265 may be implemented in a metal layer.
- a deep well-region 220 is depicted.
- the deep well-region 220 is formed below the first well-region 205 and the second well-region 210 in the p-type substrate 260, and extends uniformly between the first well-region 205 and the second well-region 210.
- the deep well-region 220 may extend to a surface of the substrate.
- the second well-region 210 is effectively formed by the deep well region, e.g. a portion of the deep well region.
- the SPAD 200 also comprises a P+ implant region 230 formed on the first wellregion 205, to define an avalanche region 235 of the SPAD 200.
- the second well-region 210 and the deep well-region 220 are configured to provide a conductive path 225 between the avalanche region 235 and the plurality of contacts 215.
- a further contact 240 is formed over the implant region 230 to define an anode of the SPAD 200.
- a p-well is formed in the p-type substrate 260 and the further contacts 270 are formed from a P+ diffused portion 280, for providing an ohmic contact to a plurality of metal contacts 285.
- FIG. 2 Also shown in Figure 2 is a plan view of the SPAD 200. In the plan view it can be seen that the second well-region 210 extends completely around the first well-region 205.
- the deep well-region 220 extends uniformly between the first wellregion 205 and the second well-region 210. That is, the deep well-region 220 extends with a uniform doping density between the first well-region 205 and the second wellregion 210, and the deep well-region 220 extends laterally in all directions between the first well-region 205 and the second well-region 210.
- the second well-region and the deep well-region are configured to provide a very low resistance conductive path 225 between the avalanche region 235, e.g. the first well-region 205, and the plurality of contacts 215.
- FIG. 3 depicts a SPAD pixel read-out circuit 300 according to an embodiment of the disclosure.
- the SPAD pixel read-out circuit 300 comprises a SPAD 305.
- the equivalent circuit of the SPAD 305 is depicted, wherein the SPAD 305 comprises an internal resistor 395 effectively coupled between a cathode of a photosensitive component of the SPAD 305 and a high voltage reference VHV.
- An anode of the SPAD 305 is coupled to a buffer 310.
- the buffer 310 represents read-out circuitry, e.g. a circuit configured to read-out a state of the SPAD.
- the SPAD pixel read-out circuit 300 is an integrated device, and as such the buffer 310 may be fabricated using low-voltage CMOS transistors.
- the buffer 310 is coupled to a supply voltage VDD.
- a voltage of the supply rail VDD is lower than a voltage of the high voltage reference VHV.
- the buffer 310 is implemented as an inverter. That is, an output of the buffer 310 represents an inverse of node C, e.g. if a voltage at node C is high, an output of the inverter is low.
- Node C corresponds to the anode of the SPAD 305
- a current mirror 315 configured to mirror a quench current IQ to the SPAD 305. That is, the current mirror 315 implements a passive quenching circuit configured to provide a constant quench current IQ. It will be understood that this is merely an example of a quenching circuit, and other quenching circuits are known in the art.
- the buffer 310 may indicate occurrence of avalanche triggering events, e.g. photon strikes, as a drop in an output voltage of the buffer 310
- the internal resistor 395 operates effectively as an internal quenching resistor.
- a quenching transistor is used with the SPAD 305, e.g. in current mirror 315.
- voltage requirements of any external quenching resistance may be reduced.
- requirements for any read-out electronics may also be reduced relative to the prior art SPAD pixel read-out circuit 100 of Figure 1, according to a resistive voltage divider formed by the effective internal quenching resistor and an effective external quenching resistance of the current mirror 315.
- the internal quenching resistor 395 enables the SPAD 305 to be operated at an excess bias voltage exceeding a maximum operating voltage for low- voltage transistors that may be used to implement the buffer 310 and the current mirror 315.
- this enables the SPAD 305 to be operated with a higher excess bias voltage, thereby improving photon detection efficiency and timing jitter, and overall product performance.
- Figure 4 depicts a plan view of a SPAD 400.
- Figure 4 also depicts a cross- sectional view of the SPAD 400 across a line B-B.
- the SPAD 400 may be implemented as the SPAD 305 in the SPAD pixel read-out circuit 300 of Figure 3.
- SPAD 400 is depicted as substantially square-shaped in plan view, it will be understood that this is for purposes of example only, and the SPAD 400 falling within the scope of the disclosure may be implemented as other shapes, such as polygonal or single-sided shapes , e.g. circular, oval-shaped, etc.
- the SPAD 400 is formed on a P-type substrate 460.
- the example SPAD comprises a first well-region 405 formed in the substrate 460.
- the first well-region 405 is denoted an “N-enhance region”, e.g. a well heavily doped with n-type impurities.
- the second well-region 410 is an N-type well, e.g. formed by diffusion of n-type impurities into the P-type substrate 460.
- a plurality of contacts 415 are formed over a portion of the second well-region 410.
- the plurality of contacts 415 comprises an N+ diffused portion, for providing an ohmic contact to a plurality of cathodes 465, where the cathodes 465 may be implemented in a metal layer.
- a guard ring 445 is provided by a lightly-doped lateral region extending between the first well-region 405 and the second well-region 410, and extending completely around the first well-region 405.
- a deep well-region 420 is depicted.
- the deep well-region 420 is formed below the first well-region 405 and only a portion of the second well-region 410 in the p-type substrate 460. That is, in contrast to the SPAD 200 of Figure 2, the deep well-region 420 extends non-uniformly between the first well-region 405 and the second wellregion 410, e.g. not extending continuously all around the first well region 405 as described in more detail below.
- the SPAD 400 also comprises a P+ implant region 430 formed on the first wellregion 405, to define an avalanche region 435 of the SPAD 400.
- the second well-region 410 and the deep well-region 420 are configured to provide conductive paths 425, 450 between the avalanche region 435 and the plurality of contacts 415.
- a further contact 440 is formed over the implant region 430 to define an anode of the SPAD 400.
- further contacts 470 to the p-type substrate 460 are also depicted.
- a p-well is formed in the p-type substrate 460 and the further contacts are formed from a P+ diffused portion 480, for providing an ohmic contact to a plurality of metal contacts 485.
- the deep wellregion 420 does not extend below the plurality of contacts 415.
- the conductive paths 425, 450 between the avalanche region 435 and the plurality of contacts 415 are indirect conductive paths 425, 450.
- the second well-region 410 and the deep wellregion 420 are not configured to provide the shortest path between the first well-region 405 and the plurality of contacts 415.
- the SPAD 400 effectively comprises a first conductive path 425 extending one way around the first well-region 405, and a second conductive path 450 extending the opposite way around the first well-region 405.
- the deep well-region 420 extending non-uniformly between the first well-region 405 and the second well-region 410 may increase an overall resistance of the conductive paths 425, 450, compared to a resistance between the first wellregion 405 and the second well-region 410 of the SPAD 200 of Figure 2.
- Such an increased resistance may effectively implement the above described internal quenching resistor 395, thereby enabling the SPAD 400 to be operated at an excess bias voltage exceeding a maximum operating voltage for low-voltage transistors that may be used to implement the readout circuit or quenching circuitry, e.g. buffer 310 and the current mirror 315.
- Figure 5 depicts a plan view of a SPAD 500.
- Figure 5 also depicts a cross- sectional view of the SPAD 500 across a line C-C.
- the SPAD 500 may be implemented as the SPAD 305 in the SPAD pixel read-out circuit 300 of Figure 3.
- the SPAD 500 is depicted as substantially square-shaped in plan view, it will be understood that this is for purposes of example only, and the SPAD 500 falling within the scope of the disclosure may be implemented as other shapes, such as polygonal or single-sided shapes.
- the SPAD 500 is formed on a P-type substrate 560.
- the example SPAD comprises a first well-region 505 formed in the substrate 560.
- the first well-region 505 is denoted an “N-enhance region”, e.g. a well heavily doped with n-type impurities.
- the second well-region 510 is an N-type well, e.g. formed by diffusion of n-type impurities into the P-type substrate 560.
- a single contact 515 is formed over a portion of the second well-region 510.
- the single contact 515 comprises an N+ diffused portion, for providing an ohmic contact to a cathode 565, where the cathode 565 may be implemented in a metal layer.
- a guard ring 545 is provided by a lightly-doped lateral region extending between the first well-region 505 and the second well-region 510, and extending completely around the first well-region 505.
- a deep well-region 520 is depicted.
- the deep well-region 520 is formed below the first well-region 505 and only a portion of the second well-region 510 in the p-type substrate 560. That is, in contrast to the SPAD 200 of Figure 2, the deep well-region 520 extends non-uniformly between the first well-region 505 and the second wellregion 510, e.g. not extending continuously all around the first well region 505 as described in more detail below.
- the SPAD 500 also comprises a P+ implant region 530 formed on the first wellregion 505, to define an avalanche region 535 of the SPAD 500.
- the second well-region 510 and the deep well-region 520 are configured to provide conductive paths 525, 550 between the avalanche region 535 and the single contact 515.
- a resistance of the conductive paths 525, 550 between the avalanche region 535 and the single contact 515 maybe increased relatively.
- a further contact 540 is formed over the implant region 530 to define an anode of the SPAD 400.
- a p-well is formed in the p-type substrate 560 and the further contacts are formed from a P+ diffused portion 580, for providing an ohmic contact to a plurality of metal contacts 585.
- the deep wellregion 520 does not extend below the single contact 515.
- only a relatively narrow portion of the deep well-region 520 extends from the first well-region 505 to the second well-region 510.
- an effective resistance of the conductive path may be increased without increasing an overall size of the SPAD 500.
- the deep well-region 520 extends below a first corner of the second well-region 510 and the single contact 515 is provided over an opposite corner of the second well-region 510, e.g.
- the resistance of the conductive paths 525 and 550 may also be maximized.
- the conductive paths 525, 550 between the avalanche region 535 and the single contact 515 are indirect conductive paths 525, 550. That is, the second wellregion 510 and the deep well-region 520 are not configured to provide the shortest path between the first well-region 505 and the plurality of contacts 515, and furthermore at least a deep well portion of the conductive paths 525, 550 is relatively narrow to increase its resistance.
- Figure 6 depicts a plan view of a SPAD 600.
- Figure 6 also depicts a cross- sectional view of the SPAD 600 across a line D-D.
- the SPAD 600 may be implemented as the SPAD 305 in the SPAD pixel read-out circuit 300 of Figure 3.
- the SPAD 600 is depicted as substantially square-shaped in plan view, it will be understood that this is for purposes of example only, and the SPAD 600 falling within the scope of the disclosure may be implemented as other shapes, such as polygonal or single-sided shapes.
- the SPAD 600 comprises: a P-type substrate 660, a first well-region 605 formed in the substrate 660; a second well-region 610 formed in the P-type substrate 660; a single contact 615 formed over a portion of the second well-region 610, wherein the single contact 615 comprises an N+ diffused portion for providing an ohmic contact to a cathode 665; a guard ring 645 provided by a lightly-doped lateral region extending between the first well-region 605 and the second well-region 610; a deep well-region 620, wherein the second well-region 610 and the deep well-region 620 are configured to provide conductive paths 625, 650 between an avalanche region 635 and the single contact 615; a P+ implant region 630 formed on the first well-region 605 to define the avalanche region 635; and a further contact 640 formed over the implant region 630 to define an anode.
- the deep well-region 620 extends non-uniformly between the first well-region 605 and the second well-region 610. That is, the deep well-region 620 extends with a non-uniform doping profile.
- the deep well region 620 is formed from a first portion of the deep well-region and a second portion of the deep well-region separated by a gap 655, wherein a lateral spread and/or thermal diffusion of the deep well-region 620 causes the conductive path 625, 650 to extend across the gap.
- the gap 655 is effectively bridged by means of lateral spread and/or thermal diffusion, such that conductive paths 625, 650 exhibit a higher effective resistance than the paths conductive paths 525, 550 of the example SPAD 500 of Figure 5.
- a size of the gap 655 may be selected to select a resistance of the conductive path.
- Figure 7 depicts a plan view of a SPAD 700.
- Figure 7 also depicts a cross- sectional view of the SPAD 700 across a line E-E.
- the SPAD 700 may be implemented as the SPAD 305 in the SPAD pixel read-out circuit 300 of Figure 3.
- the SPAD 700 is depicted as substantially square-shaped in plan view, it will be understood that this is for purposes of example only, and the SPAD 700 falling within the scope of the disclosure may be implemented as other shapes, such as polygonal or single-sided shapes.
- the SPAD 700 comprises: a P-type substrate 760 a first well-region 705 formed in the substrate 760; a second well-region 710 formed in the P-type substrate 760; a plurality of contacts 715 formed over the second well-region 710, wherein the plurality of contacts 715 comprises an N+ diffused portion for providing an ohmic contact to a plurality of cathodes 765; a guard ring 745 provided by a lightly-doped lateral region extending between the first well-region 705 and the second well-region 710; a deep well-region 720, wherein the second well-region 710 and the deep well-region 720 are configured to provide a conductive path between an avalanche region 735 and the plurality of contacts 715; a plurality of contacts 715; a P+ implant region 730 formed on the first well-region 705 to define the avalanche region 735; and a further contact 740 formed over the implant region 730 to define an anode.
- the deep well-region 620 extends non-uniformly between the first well-region 705 and the second well-region 710. That is, the deep well-region 720 extends with a non-uniform doping profile.
- the deep well region 720 is formed form a first portion of the deep well-region and a second portion of the deep well-region separated by a gap 755a, 755b, 755c, 755d, wherein a lateral spread and/or thermal diffusion of the deep well-region 720 causes the conductive path to extend across the gap.
- the second portion of the deep well-region 720 extends completely around the first portion of the deep well-region 720.
- the gap 755a, 755b, 755c, 755d extends completely around the first portion of the deep well-region 720.
- the gap 755a, 755b, 755c, 755d is effectively bridged by means of lateral spread and/or thermal diffusion, such that the conductive path exhibits a higher effective resistance than the conductive path of the example SPAD 200 of Figure 2.
- a size of the gap 755a, 755b, 755c, 755d may be selected to select a resistance of the conductive path.
- the gap 755a, 755b, 755c, 755d may extend non- uniformly around the first portion of the deep well-region 720. That is, for example, one or more portions of the gap denoted 755a, 755b, 755c, 755d in Figure 7 may be larger or smaller than at least one other portion of the gap denoted 755a, 755b, 755c, 755d in Figure 7. As a non-limiting example, the gap denoted 755a may be larger than the gap denoted 755b.
- a resistance of a conductive path extending from the avalanche region 735 and across the relatively large gap denoted 755a may be higher than a resistance of a conductive path extending across the relatively small gap denoted 755a.
- the contacts 715 e.g. the cathodes, or at least the N+ diffused portion for providing the ohmic contact, may not extend completely around the first well region. Instead, the contacts 715 may be implemented as depicted in Figure 4, wherein the N+ diffused portion only extends only partway around the first well region 705.
- the contacts 715 may be only formed in the vicinity of, e.g. adjacent, the larger gap 755a, such that any conductive path extending from the avalanche region 735 extends predominantly across the smaller gap 755b, thereby increasing an overall resistance of such a conductive path.
- having the gap 755a, 755b, 755c, 755d extending non-uniformly around the first portion of the deep well-region 720 as few as a single contact 715 may be implemented in the vicinity of, e.g. adjacent, the larger gap 755a, such as depicted in Figures 5 and 6.
- gap 755a, 755b, 755c, 755d extending non- uniformly around the first portion of the deep well-region 720, as few as a single contact 715 may be implemented in the vicinity of the largest gap(s) and no contacts may be implemented in the vicinity of the smallest gap(s).
- one or more portions of the gap denoted 755a, 755b, 755c, 755d in Figure 7 may be larger or smaller than at least one other portion of the gap denoted 755a, 755b, 755c, 755d in Figure 7, and also the deep well-region 720 extends to a surface of the substrate 760.
- the second wellregion 710 is effectively formed by the deep well region, e.g. a portion of the deep well region 720.
- any conductive path extending from the avalanche region 735 to the effective second well-region e.g.
- FIG. 8a and 8b depict arrays of SPADs 800, 860.
- the arrays of SPADs 800, 860 each only comprises four SPADs, although it will be appreciated that in other examples fewer than or greater than four SPADs may be implemented in each array.
- Figure 8a depicts a plan view of the SPAD array 800.
- the array of SPADs comprises a plurality of first well-regions 805a, 805b, 805c, 805d formed in a substrate.
- a second well-region 810 is also formed on the substrate and extends around and between each of the plurality of first well-regions 805a, 805b, 805c, 805d.
- the second well-region 810 effectively forms a grid-like structure.
- a contact 815 is formed over a central portion of the second wellregion 810, e.g. equidistant from each first well-region 805a, 805b, 805c, 805d.
- the contact 815 comprises an n+ region 880a, for providing an ohmic contact to a cathode 865a.
- a deep well-region 820 extends non-uniformly between each first well-region 805a, 805n, 805c, 805d and the second well-region 810, wherein the second wellregion and the deep well-region 820 are configured to provide conductive paths 825, 850 between avalanche regions defined by a junction with each first well-region 805a, 805b, 805c, 805d and the contact 815.
- conductive paths 825, 850 are illustrated for only one of the first well-regions 805d.
- a P+ implant region 830a, 830b, 830c, 830d is formed on each first well-region 805a, 805b, 805c, 805d, to define the avalanche regions of four SPADs.
- the deep well region 820 is formed form first portions of the deep well-region below each first well-region 805a, 805b, 805c, 805d, and a second portions of the deep well-region extending below corners of the second well-region 810 and separated by a gaps 855a, 855b, 855c, 855d, wherein a lateral spread and/or thermal diffusion of the deep well-region 820 causes the conductive paths to extend across each gap 855a, 855b, 855c, 855d.
- the deep well region 820 extends below all of the first well-regions 805a, 805b, 805c, 805d.
- the gaps 855 are effectively bridged by means of lateral spread and/or thermal diffusion, such that conductive paths 825, 850 exhibit a higher effective resistance than, for example, the paths conductive paths 525, 550 of the example SPAD 500 of Figure 5.
- a size of each gap 855a, 855b, 855c, 855d may be selected to select a resistance of the respective conductive path.
- the second well-region 810 is shared between the four SPADs of the example SPAD array 800. Furthermore, the contact 815 is also shared between the four SPADs of the example SPAD array 800.
- this may enable the deep well-region 820 to be relatively large compared to each SPAD, and more manageably implemented within the constraints of design rules.
- a majority of a voltage drop may be in the gap region, e.g. gaps 855a, 855b, 855c, 855d.
- gaps 855a, 855b, 855c, 855d may still have practically the full excess bias voltage.
- substrate contacts are omitted from Figures 8a and 8b, as each example embodiment may be a small section of a much larger array.
- Figure 8b depicts an alternative embodiment to Figure 8a.
- Features of Figure 8b generally correspond to features of Figure 8a, and therefore are not described in further detail for purposes of brevity.
- an n+ region 880b is extended between adjacent first well regions. That is, in the example of Figure 8b, the n+ region 880b effectively forms a cruciform structure. In this example, each SPAD would see the full excess bias voltage even if the three other SPADs are triggered.
- the n+ region 880b provides an ohmic contact to a single cathode 865b.
- the n+ region 880b may be filled with a plurality of such metal contacts.
- Figure 9 depicts partial cross-sections of further configurations of SPADs, which may be combined with the concepts disclosed in Figures 4 to 8 to implement further embodiments of the disclosure.
- a first SPAD configuration 900a corresponds to the SPADs of Figures 4 to 8, wherein: the first well-region 905a denoted “SPADNW” is an N-well formed in a P-type substrate 960a; a second well-region 910a denoted “NW” is formed on the substrate 960a as an N-well extending at least partway around the first wellregion 905. At least one contact 915a, is formed over the second well-region 910, and a deep well-region 920a extends non-uniformly between the first well-region 905a and the second well-region 910a.
- SPADNW is an N-well formed in a P-type substrate 960a
- NW second well-region 910a denoted “NW” is formed on the substrate 960a as an N-well extending at least partway around the first wellregion 905.
- At least one contact 915a is formed over the second well-region 910, and a deep well-region 920a extends
- the second well-region 910a and the deep well-region 920a are configured to provide a conductive path between an avalanche region and the at least one contact 915a, wherein the avalanche region is defined by a junction between the first well-region 905a and an implant region 930a formed over the first well-region 905.
- the deep wellregion 920a may extend non-uniformly between the first well-region 905a and the second well-region 910a by non-uniformities in a doping profile and/or implementation of one or more indirect conductive paths.
- An example of a second SPAD configuration 900b generally corresponds to the first SPAD configuration 900a, with the addition of a P-well guard ring 945b formed between the first well-region 905b and the second well-region 910b.
- a first well-region 905c is implemented as a P-well, such that a PN junction providing the avalanche region of the SPAD may be formed between a deep-well region 920c and the first well-region 905c.
- a P+ implant region 930c is formed completely within the first wellregion 905.
- An example of a fourth SPAD configuration 900d generally corresponds to the third SPAD configuration 900c, with the addition of a SPAD N-well 975 formed within the deep N-well and below the first well-region, such that a PN junction forming the avalanche region is formed between the SPAD N-well 975 and the first well-region 905d.
- the deep well-region 920a, 920b, 920c, 920d may extend non-uniformly between the first well-region 905a, 905b, 905c, 905dand the second well-region 910a, 910b, 910c, 91 Od, wherein non-uniformities are in a doping profile and/or lateral direction of one or more indirect conductive paths formed between a respective avalanche region and the respective second well-region 910a, 910b, 910c, 910d .
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| US18/860,009 US20250301816A1 (en) | 2022-05-06 | 2023-05-03 | Single-photon avalanche diode |
| DE112023002112.0T DE112023002112T5 (en) | 2022-05-06 | 2023-05-03 | SINGLE-PHOTON AVALANCHE DIODE |
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| US (1) | US20250301816A1 (en) |
| DE (1) | DE112023002112T5 (en) |
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| WO2026079608A1 (en) * | 2024-10-10 | 2026-04-16 | 엘지이노텍 주식회사 | Single-photon avalanche diode comprising p-doped region and 1-side spot ohmic metal contact |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20170131143A1 (en) * | 2014-07-02 | 2017-05-11 | Andreas G. Andreou | Photodetection circuit and operating method thereof |
| US20180026147A1 (en) * | 2016-07-21 | 2018-01-25 | Omnivision Technologies, Inc. | Vertical gate guard ring for single photon avalanche diode pitch minimization |
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| EP2144303B1 (en) * | 2008-07-10 | 2013-02-06 | STMicroelectronics (Research & Development) Limited | Improvements in Single Photon Avalanche Diodes |
| EP3435422B1 (en) * | 2017-07-26 | 2020-05-06 | ams AG | Spad device for excess bias monitoring |
| US10985201B2 (en) * | 2018-09-28 | 2021-04-20 | Taiwan Semiconductor Manufacturing Co., Ltd. | Image sensor including silicon over germanium layer |
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2023
- 2023-04-25 TW TW112115351A patent/TWI882322B/en active
- 2023-05-03 WO PCT/EP2023/061658 patent/WO2023213872A1/en not_active Ceased
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20170131143A1 (en) * | 2014-07-02 | 2017-05-11 | Andreas G. Andreou | Photodetection circuit and operating method thereof |
| US20180026147A1 (en) * | 2016-07-21 | 2018-01-25 | Omnivision Technologies, Inc. | Vertical gate guard ring for single photon avalanche diode pitch minimization |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2026079608A1 (en) * | 2024-10-10 | 2026-04-16 | 엘지이노텍 주식회사 | Single-photon avalanche diode comprising p-doped region and 1-side spot ohmic metal contact |
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| DE112023002112T5 (en) | 2025-02-20 |
| TW202349736A (en) | 2023-12-16 |
| US20250301816A1 (en) | 2025-09-25 |
| TWI882322B (en) | 2025-05-01 |
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