WO2011117309A2 - Silicon photomultiplier and readout method - Google Patents

Silicon photomultiplier and readout method Download PDF

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Publication number
WO2011117309A2
WO2011117309A2 PCT/EP2011/054475 EP2011054475W WO2011117309A2 WO 2011117309 A2 WO2011117309 A2 WO 2011117309A2 EP 2011054475 W EP2011054475 W EP 2011054475W WO 2011117309 A2 WO2011117309 A2 WO 2011117309A2
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Prior art keywords
electrode
silicon photomultiplier
signal
output signal
photosensitive cells
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PCT/EP2011/054475
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French (fr)
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WO2011117309A3 (en
Inventor
Nikolai Pavlov
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Sensl Technologies Ltd
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Priority to US13/636,720 priority Critical patent/US9029772B2/en
Priority to EP11710190A priority patent/EP2550548A2/en
Publication of WO2011117309A2 publication Critical patent/WO2011117309A2/en
Publication of WO2011117309A3 publication Critical patent/WO2011117309A3/en

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    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L27/00—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate
    • H01L27/14—Devices consisting of a plurality of semiconductor or other solid-state components formed in or on a common substrate including semiconductor components sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation
    • H01L27/144—Devices controlled by radiation
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16—Measuring radiation intensity
    • G01T1/24—Measuring radiation intensity with semiconductor detectors
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/08—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors
    • H01L31/10—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors characterised by potential barriers, e.g. phototransistors
    • H01L31/101—Devices sensitive to infrared, visible or ultraviolet radiation
    • H01L31/102—Devices sensitive to infrared, visible or ultraviolet radiation characterised by only one potential barrier
    • H01L31/107—Devices sensitive to infrared, visible or ultraviolet radiation characterised by only one potential barrier the potential barrier working in avalanche mode, e.g. avalanche photodiodes
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16—Measuring radiation intensity
    • G01T1/24—Measuring radiation intensity with semiconductor detectors
    • G01T1/248—Silicon photomultipliers [SiPM], e.g. an avalanche photodiode [APD] array on a common Si substrate
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/08—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors
    • H01L31/09—Devices sensitive to infrared, visible or ultraviolet radiation

Definitions

  • the present invention relates to photon detectors.
  • the present invention relates to fast, high sensitivity photon detectors such as silicon photomultipliers, and to a readout method for silicon photomultipliers.
  • the present invention relates to silicon photomultipliers (SiPMs or SPMs) in such areas as Positron Emission Tomography [PET], including Time-Of-Flight PET [TOF-PET], Laser Ranging [LIDAR] applications, bio luminescence, High Energy Physics [HEP] detectors.
  • PET Positron Emission Tomography
  • TOF-PET Time-Of-Flight PET
  • LIDAR Laser Ranging
  • HEP High Energy Physics
  • SPMs are silicon photon sensitive devices made up of an array of very small Geiger- mode avalanche photodiode (APD) cells on a silicon substrate.
  • An example 10 x 10 microcell array is shown in Figure 1 of the accompanying drawings. Each cell is connected to one another to form one larger device with one signal output. The entire device size can be as small as 1 ⁇ 1 mm or much larger.
  • Figure 2 of the accompanying drawings is a schematic diagram of a conventional silicon photomultiplier.
  • APD cells vary in dimension from 20 to 100 microns depending on the mask used, and can have a density of up to 1000/sq. mm.
  • Avalanche diodes can also be made from other semiconductors besides silicon, depending on the properties that are desirable. Silicon detects in the visible and near infrared range, with low multiplication noise (excess noise). Germanium (Ge) detects infrared to 1.7 ⁇ wavelength, but has high multiplication noise. InGaAs (Indium Gallium Arsenide) detects to a maximum wavelength of 1.6 um, and has less multiplication noise than Ge.
  • InGaAs is generally used for the multiplication region of a heterostructure diode, is compatible with highspeed telecommunications using optical fibers, and can reach speeds of greater than Gbit/s.
  • Gallium nitride operates with UV light.
  • HgCdTe Mercury Cadmium Telluride
  • HgCdTe Mercury Cadmium Telluride
  • Silicon avalanche diodes can function with breakdown voltages of 100 to 2000V, typically.
  • APDs exhibit internal current gain effect of about 100-1000 due to impact ionization, or avalanche effect, when a high reverse bias voltage is applied (approximately 100-200 V in silicon).
  • Greater voltage can be applied to silicon APDs, which are more sensitive compared to other semiconductor photodiodes, than to traditional APDs before achieving breakdown allowing for a larger operating gain, preferably over 1000, because silicon APDs provide for alternative doping.
  • Reverse voltage is proportional to gain, and APD gain also varies dependent ly on both reverse bias and temperature, which is why reverse voltage should be controlled in order to preserve stable gain.
  • SPMs can achieve a gain of 10 5 to 10 6 by using Geiger mode APDs which operate with a reverse voltage that is greater than the breakdown voltage, and by maintaining the dark count event rate at a sufficiently low level.
  • Geiger-mode APDs produce relatively large charge pulse when struck by a photon of the same amplitude no matter the energy of the photon.
  • noise of the preamplifier significantly degrades timing and amplitude resolution performance for short (shorter then approx 500ns) light pulses.
  • SPMs using Geiger mode APDs provide much higher output amplitude, essentially eliminating the impact of preamplifier noise.
  • SiPM Silicon Photomultiplier
  • SPM Silicon Photomultiplier
  • MPPC MicroPixel Photon Counters
  • MPD MicroPixel Avalanche Photodiodes
  • PET Positron Emission Tomography
  • TOF-PET Time-Of-Flight PET
  • LIDAR Laser Ranging
  • HEP High Energy Physics
  • Currently known Silicon Photomultipliers provide minimum output risetime of order of InS and fall time of at least 10ns. This is much longer than conventional vacuum Photomultiplier (PMTs) or silicon avalanche photodiodes (APDs) resulting in performance loss and complication of readout electronics.
  • An embodiment of the present invention proposes a third electrode to be used as signal output while two other electrodes are maintained for biasing and signal ground.
  • the third electrode affords a dramatic reduction in both the fall and rise time of the signal.
  • An embodiment of the present invention provides a three electrode silicon photomultiplier having output pulses of short duration and thereof readout method.
  • a third readout electrode is proposed to be introduced in some version of the SPM.
  • This electrode is insulated by Silicon Oxide or another dielectric from all the elements of the SPM structure but has weak capacitive coupling to each photocell.
  • Such capacitive coupling provides fast, partial (1-10% or so) injection of the signal charge (which is of the order of 0.15 pC/photocell) when the photocell is firing.
  • the capacitance of the third electrode toward other electrodes of the SPM stays rather low, of the order of 10% of total SPM capacitance.
  • a transparent conductor for example very thin gold, transparent conducting oxide such as Indium Tin Oxide
  • a grid-like structure comprising a non-transparent conductor may be used.
  • a silicon photomultiplier device comprising a first electrode arranged to provide a bias voltage to the device, a second electrode arranged as a ground electrode, and a third electrode arranged to provide an output signal from the device using the second electrode as the output signal ground.
  • the third electrode may be galvanically isolated from the first and second electrode.
  • the signal in the third electrode may be induced electrostatically.
  • the device may comprise a plurality of avalanche photodiodes.
  • the device may comprise a plurality of Geiger mode avalanche photodiodes.
  • the third electrode may be coupled to a cathode of the photodiode, for example via a capacitive coupling.
  • the signal in the third electrode may be induced by capacitive coupling between the third electrode and the photodiode cathodes.
  • the capacitance of the third electrode with the photodiode cathodes may be between 2% and 20% of the total silicon photomultiplier capacitance.
  • the capacitance of the third electrode with the photodiode cathodes may be approximately 10%.
  • a method for reading out a silicon photomultiplier device comprising reading out the output signal from the third electrode using a current integrating charge amplifier to provide an output proportional to the number of photodiodes firing within a period of time of interest.
  • Figure 1 illustrates the structure of a silicon photomultiplier
  • FIG. 2 is a schematic diagram of a conventional silicon photomultiplier
  • Figure 3 is a schematic diagram of a silicon photomultiplier with a third readout electrode according to an embodiment of the present invention
  • Figure 4 is an equivalent schematic circuit for simulation of a silicon photomultiplier with 3600 photocells
  • Figure 5 is the result of a simulation carried out using the schematic of Figure 4, comparing response time using a conventional readout and from the third readout electrode.
  • a silicon photomultiplier comprising an array of Geiger mode photodiodes is shown.
  • the array is formed on a semiconductor substrate using semiconductor processes which will be known to one skilled in the art.
  • Patterned layers of conducting material, insulating material and doped areas of semiconductor form the structure of the photodiode.
  • a resistor is provided adjacent to each photodiode which may be used to limit the avalanche current.
  • the photodiodes are electrically connected to common biasing and ground electrodes by aluminium tracking.
  • FIG. 2 An equivalent circuit schematic is shown in Figure 2 for a conventional silicon photomultiplier in which the anodes of an array of photodiodes are connected to a common ground electrode and the cathodes of the array are connected via current limiting resistors to a common bias electrode for applying a bias voltage across the diodes.
  • Figure 3 an arrangement according to an embodiment of the invention is shown in which a third electrode is capacitively coupled each photodiode cathode to provide a fast readout of the avalanche signals from the photodiodes. When the photodiode emits a current pulse, part of the resulting change in voltage at the cathode will be coupled via mutual capacitance into the third electrode. Using a third electrode for readout avoids the compromised transient performance resulting from the relatively large RC time constant associated with the biasing circuit.
  • Figure 4 shows an equivalent circuit which is used to illustrate the performance advantage of an embodiment of the invention.
  • the current source II represents the avalanche current of the diode, CI the capacitance of the photodiode and C5 the capacitance between the third electrode and the photodiode.
  • the remaining network represents a previously considered biasing circuit and readout approach. In a previously- considered readout the current through R3 simulates the readout, while the current through R7 simulates the readout according to an embodiment of the present invention.
  • Figure 5 shows the results of a simulation comparing the rise and fall times of the currents through R3 and R7 resulting from the injection of a transient avalanche current at II. It is clear that the current through R7 responds more quickly in both rise and fall than the current through R3, clearly demonstrating the advantage of the embodiment of the invention.
  • An embodiment of the present invention can overcome the problems and disadvantages associated with current strategies and designs and provides new materials and methods for improving photodetectors such as SPM devices.
  • SPMs have the potential to become a replacement for photomultiplier tubes (PMTs) and avalanche photodiode (APDs) for use as photodetectors in positron emission topography (PET), Single photon emission computed tomography (SPECT), computed tomography (CT), and other radiation detectors.
  • PMTs photomultiplier tubes
  • APDs avalanche photodiode
  • PET positron emission topography
  • SPECT Single photon emission computed tomography
  • CT computed tomography
  • These devices are compact, have high gain, high quantum efficiency (about 20%-70%, which is better than that of traditional PMTs) and low noise.
  • These devices have the potential to be used in time-of- flight PET applications due to their potential timing performance. They are also insensitive to magnetic fields, a quality which makes them ideal for use in an MR (magnetic resonance) environment.
  • One embodiment of this invention is directed to a silicon photomultiplier (SPM) device comprising a three electrode connection scheme where two electrodes are used for biasing of the SPM and as the signal and ground electrodes, while a third electrode is used to read out the signal, using one of the first two electrodes as signal ground.
  • the third electrode is galvanically isolated from the first two electrodes and capacitively coupled to each Geiger-mode photosensitive cell.
  • the SPM device comprises an array of Geiger-mode avalanche photodiode (APD) cells wherein the array produces an output pulse proportional to an input photon pulse.
  • APD Geiger-mode avalanche photodiode
  • Another embodiment is directed to the readout method of a three electrode SPM device, wherein the third (signal) electrode is read out using wideband (bandwidth > 200MHz) amplifier with low input impedance ( ⁇ 200 ohm) proving output pulses with less then 5nS duration.
  • Another embodiment is directed to the readout method of a three electrode SPM device, where the third (signal) electrode is read out using a charge sensitive (current integrating) amplifier providing an output proportional to the number of Geiger-mode photosensitive cells firing within some period of time of interest.
  • an embodiment of the present invention provides a silicon photomultiplier [SPM] device having a three electrode connection scheme where two electrodes are used for biasing of the SPM and as the signal ground electrode, while a third electrode is used to readout the signal using one of the first two electrodes as signal ground.
  • SPM silicon photomultiplier
  • the third electrode may be galvanically isolated from first two electrodes and capacitively coupled to each Geiger-mode photosensitive cell.
  • the signal in the third electrode may be induced electrostatically.
  • the third (signal) electrode may be read out using wideband (e.g. bandwith > 200MHz) amplifier with low input impedance (e.g. ⁇ 200 ohm) providing output pulses with less than e.g. 5ns duration.
  • the third (signal) electrode may be read out using charge sensitive (current integrating) amplifier providing an output proportional to the number of Geiger-mode photosensitive cells firing within a period of time of interest.

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Abstract

Silicon photomultiplier and readout method A silicon photomultiplier device is provided which comprises a first electrode arranged to provide a bias voltage to the device, a second electrode arranged as a ground electrode for the device, and a third electrode arranged to provide an output signal from the device using the second electrode as the output signal ground.

Description

SILICON PHOTOMULTIPLIER AND READOUT METHOD
The present invention relates to photon detectors. In particular, the present invention relates to fast, high sensitivity photon detectors such as silicon photomultipliers, and to a readout method for silicon photomultipliers. In particular, but not exclusively, the present invention relates to silicon photomultipliers (SiPMs or SPMs) in such areas as Positron Emission Tomography [PET], including Time-Of-Flight PET [TOF-PET], Laser Ranging [LIDAR] applications, bio luminescence, High Energy Physics [HEP] detectors.
SPMs are silicon photon sensitive devices made up of an array of very small Geiger- mode avalanche photodiode (APD) cells on a silicon substrate. An example 10x 10 microcell array is shown in Figure 1 of the accompanying drawings. Each cell is connected to one another to form one larger device with one signal output. The entire device size can be as small as 1 χ1 mm or much larger. Figure 2 of the accompanying drawings is a schematic diagram of a conventional silicon photomultiplier.
APD cells vary in dimension from 20 to 100 microns depending on the mask used, and can have a density of up to 1000/sq. mm. Avalanche diodes can also be made from other semiconductors besides silicon, depending on the properties that are desirable. Silicon detects in the visible and near infrared range, with low multiplication noise (excess noise). Germanium (Ge) detects infrared to 1.7 μιη wavelength, but has high multiplication noise. InGaAs (Indium Gallium Arsenide) detects to a maximum wavelength of 1.6 um, and has less multiplication noise than Ge. InGaAs is generally used for the multiplication region of a heterostructure diode, is compatible with highspeed telecommunications using optical fibers, and can reach speeds of greater than Gbit/s. Gallium nitride operates with UV light. HgCdTe (Mercury Cadmium Telluride) operates in the infrared, to a maximum wavelength of about 14 μιη, requires cooling to reduce dark currents, and can achieve a very low level of excess noise.
Silicon avalanche diodes can function with breakdown voltages of 100 to 2000V, typically. APDs exhibit internal current gain effect of about 100-1000 due to impact ionization, or avalanche effect, when a high reverse bias voltage is applied (approximately 100-200 V in silicon). Greater voltage can be applied to silicon APDs, which are more sensitive compared to other semiconductor photodiodes, than to traditional APDs before achieving breakdown allowing for a larger operating gain, preferably over 1000, because silicon APDs provide for alternative doping. Reverse voltage is proportional to gain, and APD gain also varies dependent ly on both reverse bias and temperature, which is why reverse voltage should be controlled in order to preserve stable gain. SPMs can achieve a gain of 10 5 to 10 6 by using Geiger mode APDs which operate with a reverse voltage that is greater than the breakdown voltage, and by maintaining the dark count event rate at a sufficiently low level.
Geiger-mode APDs produce relatively large charge pulse when struck by a photon of the same amplitude no matter the energy of the photon. When reading out conventional APDs, noise of the preamplifier significantly degrades timing and amplitude resolution performance for short (shorter then approx 500ns) light pulses. Comparing to conventional APDs, SPMs using Geiger mode APDs provide much higher output amplitude, essentially eliminating the impact of preamplifier noise.
Many SPM [Silicon Photomultiplier] applications call for a fast light-to-current response, with order of Ins or even shorter time constants. Improved time response would benefit such applications as time-resolved spectroscopy, LIDARs, TOF [time of flight] PET [Positron Emission Tomography] etc.
At the moment use of the SPM for 'fast' applications, especially large area SPMs is seriously compromised by the fact that bulk of the SPM's signal charge is released as exponentially an decaying current with a long ~50ns time constant. However, the avalanche development process in the SPM APD is extremely fast and the long time constant arises due to the fact that the APD signals are read out through the distributed SPM's biasing circuitry.
It is desirable to provide new electrode detector configurations to enhance currently known Silicon Photomultiplier [SiPM], also known as SPM, MicroPixel Photon Counters [MPPC], MicroPixel Avalanche Photodiodes [MAPD] with improved performance in such areas as Positron Emission Tomography [PET], including Time-Of-Flight PET [TOF-PET], Laser Ranging [LIDAR] applications, bio luminescence, High Energy Physics [HEP] detectors. Currently known Silicon Photomultipliers provide minimum output risetime of order of InS and fall time of at least 10ns. This is much longer than conventional vacuum Photomultiplier (PMTs) or silicon avalanche photodiodes (APDs) resulting in performance loss and complication of readout electronics.
An embodiment of the present invention proposes a third electrode to be used as signal output while two other electrodes are maintained for biasing and signal ground. The third electrode affords a dramatic reduction in both the fall and rise time of the signal.
An embodiment of the present invention provides a three electrode silicon photomultiplier having output pulses of short duration and thereof readout method.
According to an embodiment of the present invention, a third readout electrode is proposed to be introduced in some version of the SPM. This electrode is insulated by Silicon Oxide or another dielectric from all the elements of the SPM structure but has weak capacitive coupling to each photocell. Such capacitive coupling provides fast, partial (1-10% or so) injection of the signal charge (which is of the order of 0.15 pC/photocell) when the photocell is firing. The capacitance of the third electrode toward other electrodes of the SPM stays rather low, of the order of 10% of total SPM capacitance. To implement this electrode, either a transparent conductor (for example very thin gold, transparent conducting oxide such as Indium Tin Oxide) or a grid-like structure comprising a non-transparent conductor may be used. According to a first aspect of the invention, there is provided a silicon photomultiplier device comprising a first electrode arranged to provide a bias voltage to the device, a second electrode arranged as a ground electrode, and a third electrode arranged to provide an output signal from the device using the second electrode as the output signal ground. The third electrode may be galvanically isolated from the first and second electrode. The signal in the third electrode may be induced electrostatically.
The device may comprise a plurality of avalanche photodiodes. The device may comprise a plurality of Geiger mode avalanche photodiodes.
The third electrode may be coupled to a cathode of the photodiode, for example via a capacitive coupling. The signal in the third electrode may be induced by capacitive coupling between the third electrode and the photodiode cathodes. The capacitance of the third electrode with the photodiode cathodes may be between 2% and 20% of the total silicon photomultiplier capacitance. The capacitance of the third electrode with the photodiode cathodes may be approximately 10%. According to a second aspect of the invention there is provided a method of reading out a silicon photomultiplier device according to the first aspect of the present invention, comprising reading out the output signal from the third electrode using a wideband amplifier with low input impedance. The wideband amplifier may have a bandwidth greater than 200MHz and may have an input impedance of less than 200ohms.
According to a third aspect of the invention there is provided a method for reading out a silicon photomultiplier device according the first aspect of the invention, comprising reading out the output signal from the third electrode using a current integrating charge amplifier to provide an output proportional to the number of photodiodes firing within a period of time of interest.
Figure 1, discussed hereinbefore, illustrates the structure of a silicon photomultiplier;
Figure 2, also discussed hereinbefore, is a schematic diagram of a conventional silicon photomultiplier;
Figure 3 is a schematic diagram of a silicon photomultiplier with a third readout electrode according to an embodiment of the present invention; Figure 4 is an equivalent schematic circuit for simulation of a silicon photomultiplier with 3600 photocells; and
Figure 5 is the result of a simulation carried out using the schematic of Figure 4, comparing response time using a conventional readout and from the third readout electrode.
Referring to Figure 1, a silicon photomultiplier comprising an array of Geiger mode photodiodes is shown. The array is formed on a semiconductor substrate using semiconductor processes which will be known to one skilled in the art. Patterned layers of conducting material, insulating material and doped areas of semiconductor form the structure of the photodiode. As illustrated, a resistor is provided adjacent to each photodiode which may be used to limit the avalanche current. The photodiodes are electrically connected to common biasing and ground electrodes by aluminium tracking.
An equivalent circuit schematic is shown in Figure 2 for a conventional silicon photomultiplier in which the anodes of an array of photodiodes are connected to a common ground electrode and the cathodes of the array are connected via current limiting resistors to a common bias electrode for applying a bias voltage across the diodes. In Figure 3 an arrangement according to an embodiment of the invention is shown in which a third electrode is capacitively coupled each photodiode cathode to provide a fast readout of the avalanche signals from the photodiodes. When the photodiode emits a current pulse, part of the resulting change in voltage at the cathode will be coupled via mutual capacitance into the third electrode. Using a third electrode for readout avoids the compromised transient performance resulting from the relatively large RC time constant associated with the biasing circuit.
Figure 4 shows an equivalent circuit which is used to illustrate the performance advantage of an embodiment of the invention. The current source II represents the avalanche current of the diode, CI the capacitance of the photodiode and C5 the capacitance between the third electrode and the photodiode. The remaining network represents a previously considered biasing circuit and readout approach. In a previously- considered readout the current through R3 simulates the readout, while the current through R7 simulates the readout according to an embodiment of the present invention.
Figure 5 shows the results of a simulation comparing the rise and fall times of the currents through R3 and R7 resulting from the injection of a transient avalanche current at II. It is clear that the current through R7 responds more quickly in both rise and fall than the current through R3, clearly demonstrating the advantage of the embodiment of the invention. An embodiment of the present invention can overcome the problems and disadvantages associated with current strategies and designs and provides new materials and methods for improving photodetectors such as SPM devices.
SPMs have the potential to become a replacement for photomultiplier tubes (PMTs) and avalanche photodiode (APDs) for use as photodetectors in positron emission topography (PET), Single photon emission computed tomography (SPECT), computed tomography (CT), and other radiation detectors. These devices are compact, have high gain, high quantum efficiency (about 20%-70%, which is better than that of traditional PMTs) and low noise. These devices have the potential to be used in time-of- flight PET applications due to their potential timing performance. They are also insensitive to magnetic fields, a quality which makes them ideal for use in an MR (magnetic resonance) environment.
One embodiment of this invention is directed to a silicon photomultiplier (SPM) device comprising a three electrode connection scheme where two electrodes are used for biasing of the SPM and as the signal and ground electrodes, while a third electrode is used to read out the signal, using one of the first two electrodes as signal ground. The third electrode is galvanically isolated from the first two electrodes and capacitively coupled to each Geiger-mode photosensitive cell. Preferably, the SPM device comprises an array of Geiger-mode avalanche photodiode (APD) cells wherein the array produces an output pulse proportional to an input photon pulse.
Another embodiment is directed to the readout method of a three electrode SPM device, wherein the third (signal) electrode is read out using wideband (bandwidth > 200MHz) amplifier with low input impedance (<200 ohm) proving output pulses with less then 5nS duration.
Another embodiment is directed to the readout method of a three electrode SPM device, where the third (signal) electrode is read out using a charge sensitive (current integrating) amplifier providing an output proportional to the number of Geiger-mode photosensitive cells firing within some period of time of interest.
In summary, an embodiment of the present invention provides a silicon photomultiplier [SPM] device having a three electrode connection scheme where two electrodes are used for biasing of the SPM and as the signal ground electrode, while a third electrode is used to readout the signal using one of the first two electrodes as signal ground.
The third electrode may be galvanically isolated from first two electrodes and capacitively coupled to each Geiger-mode photosensitive cell. The signal in the third electrode may be induced electrostatically.
In a readout method for such a SPM device, the third (signal) electrode may be read out using wideband (e.g. bandwith > 200MHz) amplifier with low input impedance (e.g. < 200 ohm) providing output pulses with less than e.g. 5ns duration. In a readout method for such a SPM device, the third (signal) electrode may be read out using charge sensitive (current integrating) amplifier providing an output proportional to the number of Geiger-mode photosensitive cells firing within a period of time of interest.
It will be appreciated that reference herein to a three electrode connection scheme does not preclude the possibility that the device has a fourth and possibly further electrodes provided for other purposes.
It will be appreciated by the person of skill in the art that various modifications may be made to the above described embodiments without departing from the scope of the present invention.

Claims

1. A silicon photomultiplier device comprising a first electrode arranged to provide a bias voltage to the device, a second electrode arranged as a ground electrode for the device, and a third electrode arranged to provide an output signal from the device using the second electrode as the output signal ground.
2. A device according to claim 1, wherein the third electrode is galvanically isolated from the first and second electrode.
3. A device according to claim 1 or 2, being adapted to induce the output signal in the third electrode electrostatically.
4. A device according to any preceding claim, comprising a plurality of photosensitive cells, wherein the first electrode is arranged to provide a bias voltage to the photosensitive cells, the second electrode is arranged as a ground electrode for the photosensitive cells, and the third electrode is arranged to provide an output signal from the photosensitive cells.
5. A device according to claim 4, wherein the output signal in the third electrode is induced by capacitive coupling between the third electrode and the photosensitive cells.
6. A device according to claim 5, wherein the capacitance of the capacitive coupling is between 2% and 20% of a total capacitance for the device.
7. A device according to claim 6, wherein the capacitance of the capacitive coupling is approximately 10% of the total capacitance.
8. A device according to any one of claims 4 to 7, wherein each photosensitive cell comprises an avalanche photodiode.
9. A device according to claim 8, wherein the avalanche photodiode is a Geiger mode avalanche photodiode.
10. A method of reading out a silicon photomultiplier device according to any preceding claim, comprising reading out the output signal from the third electrode using a wideband amplifier with low input impedance.
11. A method according to claim 10, wherein the wideband amplifier is one having a bandwidth greater than 200MHz.
12. A method according to claim 10 or 11, wherein the wideband amplifier is one having an input impedance of less than 200 ohms.
13. A method of reading out a silicon photomultiplier device according to any of claims 1 to 9, comprising reading out the output signal from the third electrode using a current integrating amplifier to provide an output proportional to the number of photosensitive cells of the device firing within a period of time of interest.
14. A silicon photomultiplier device having a three electrode connection scheme in which two (of the three) electrodes are used for biasing of the silicon photomultiplier and as the signal ground electrode, with a third (of the three electrodes) being used to read out the signal using one of the first two electrodes as signal ground.
15. A device according to claim 14, wherein the third electrode is galvanically isolated from first two electrodes and capacitively coupled to each Geiger-mode photosensitive cell of the silicon photomultiplier.
16. A device according to claim 14 or 15, wherein the signal in the third electrode is induced electrostatically.
17. Areadout method for a silicon photomultiplier device according to claim 14, 15 or 16, wherein the third (signal) electrode is read out using a wideband (for example bandwith > 200MHz) amplifier with low input impedance (for example < 200 ohm) providing output pulses with less than for example 5ns duration.
18. A readout method for a silicon photomultiplier device according to claim 14, 15 or 16, wherein the third (signal) electrode is read out using a charge sensitive (current integrating) amplifier providing an output proportional to the number of Geiger-mode photosensitive cells firing within a period of time of interest.
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