CN109253807A - Based on standard integrated circuit technology low noise single photon detection chip and system - Google Patents

Based on standard integrated circuit technology low noise single photon detection chip and system Download PDF

Info

Publication number
CN109253807A
CN109253807A CN201811182461.XA CN201811182461A CN109253807A CN 109253807 A CN109253807 A CN 109253807A CN 201811182461 A CN201811182461 A CN 201811182461A CN 109253807 A CN109253807 A CN 109253807A
Authority
CN
China
Prior art keywords
photon
avalanche
detection
avalanche diode
signal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201811182461.XA
Other languages
Chinese (zh)
Other versions
CN109253807B (en
Inventor
邓仕杰
滕传新
刘厚权
张文涛
苑立波
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Chuanzhou Semiconductor Technology Shanghai Co ltd
Original Assignee
Guilin University of Electronic Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Guilin University of Electronic Technology filed Critical Guilin University of Electronic Technology
Priority to CN201811182461.XA priority Critical patent/CN109253807B/en
Publication of CN109253807A publication Critical patent/CN109253807A/en
Application granted granted Critical
Publication of CN109253807B publication Critical patent/CN109253807B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J11/00Measuring the characteristics of individual optical pulses or of optical pulse trains

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)
  • Light Receiving Elements (AREA)

Abstract

The present invention is to provide one kind to be based on standard integrated circuit technology low noise single photon detection chip and system.It is characterized in that: low noise single-photon detection system is made of light source 1, bias circuit 2, single photon detection chip 3, signal processing system 4, the single-photon avalanche diode 32 and avalanche events detection circuit array 33 run under single-photon avalanche diode 31 that wherein single photon detection chip 3 is run by normal mode, dark situation is formed.The present invention can be used for the measurement of atomic dim light, can be widely used for laser radar, DNA sequencing, the fields such as the distribution of quantum secret key and medical imaging.

Description

Based on standard integrated circuit technology low noise single photon detection chip and system
(1) technical field
The present invention relates to one kind to be based on standard integrated circuit technology low noise single photon detection chip and system, can use In laser radar, DNA sequencing, the detection of the poles dim light such as the distribution of quantum secret key and medical imaging belongs to detecting technique neck Domain.
(2) background technique
Single-photon detecting survey technology is a kind of detecting technique, and principle is using photoelectric effect, to incident single photon It is counted, to realize the detection to atomic weak signal.It is atomic dim light measurement such as laser ranging, DNA sequencing, and quantum is close Spoon distribution, the core of laser radar and medical imaging.As the progress and IC design of semiconductor process technique are horizontal Raising, using standard integrated circuit technology design single-photon avalanche diode (Single Photon Avalanche Diode) and by single-photon avalanche diode and relevant integrated circuit such as avalanche events sensor circuit, quenching circuit, and Back end signal processing circuit etc. is integrated to be possibly realized on the same chip.Compared to traditional single-photon detectors such as photomultiplier transit Manage (Photomultiplier Tube, PMT) or microchannel plate (Microchannel plate, MCP), such product It running under lower bias voltage, there is smaller volume, lower power consumption is insensitive for electromagnetic noise, integrated level height, It is low in cost, it is reproducible, it has broad application prospects.
In photon detection/imaging system based on single-photon avalanche diode, system passes through to two pole of single-photon avalanche The avalanche events that the hole-electron pair generated inside pipe is excited are detected and are counted.Snowslide in single-photon avalanche diode Breakdown events can not only be excited by photonic absorption, it is also possible to be excited by other factors.The snowslide being excited under no light condition Event is unrelated with photonic absorption, is referred to as dark counting to the counting of these avalanche events.Dark count rate is two pole of single-photon avalanche One important parameter of pipe, high dark count rate can reduce the signal-to-noise ratio of monochromatic light subsystem, increase error rate of system, increase imaging (exposure) time of integral needed for system and reduction detectivity.Therefore, the dark count rate in single-photon avalanche diode It needs to be reduced as far as possible.
In the integrated circuit technology of standard, for the injection depth of each layer, dopant concentration has solid chip foundries Calibration is quasi-, also has certain limitation (such as density metal) for design rule, this causes in standard integrated circuit technology The depletion layer for the single-photon avalanche diode prepared is narrow, is easy to be influenced by thermal excitation and tunnel-effect carrier, There is higher dark count rate.In addition to this, due to lacking high annealing and going defect processing step, in two pole of single-photon avalanche Higher impurity concentration can be generated around the photosensitive region of pipe, generate higher dark counting therewith.
In order to reduce the noise of single-photon detection system, researcher devises in different standard integrated circuit technologies The single-photon avalanche diode chip of different structure promotes chip to the signal-to-noise ratio of single photon detection to reduce dark count rate.Such as The photosensitive area that R.K.Henderson etc. is prepared under the technique of 90nm is 3.1 μm2Single-photon avalanche diode output Dark counting is 250Hz (R.K.Henderson, et al., " A 3 × 3,5 μm of pitch, 3-transistor single photon avalanche diode array with integrated 11 V bias generation in 90nm CMOS technology,”IEEE International Electron Devices Meeting(IEDM), pp.14.2.1–14.2.4.Dec.2010.);E.A.G.Webster is by using the p- in 90nm CMOS technology Epitaxial layers and deep n-well layers are formed to constitute single-photon avalanche diode using p-epitaxial layers Protection ring is mixed using its low to alleviate tunnel-effect.Their design reduces the dark counting of device to a certain extent Rate (E.A.G.Webster, et al., " A single-photon avalanche diode in 90-nm CMOS Imaging technology with 44%photon detection efficiency at 690nm, " IEEE Electron Device Letters.,33(5):694–696,May 2012.).Although by structure optimization, single photon detection The dark count rate of device chip has obtained a degree of alleviation, however its universal dark count rate has still reached single single photon The dozens to hundreds of Hz of avalanche diode, this makes when it is applied to single-photon avalanche diode array, and global noise is still It is very considerable.In addition to this, once peaceful to disclose " the high time resolution low noise single-photon detecting of optical pulse synchronization equal to 2010 Survey device " (Chinese patent: 201010292821.9), Gauss electricity is converted optical signal into using optical time delay unit and photoelectric conversion module Signal reduces the noise that avalanche diode is caused by capacity effect as portal vein pulsed light signal, improves signal-to-noise ratio;Zhao Yan It is vertical be equal to disclose " a kind of gate difference single-photon detection system " within 2015 and (Chinese patent: 201510413840.5), pass through Feedback control mechanism is gated, the spike noise and afterpulse effect of system is reduced, improves look-in frequency;Huang Zinan is equal to Disclose within 2016 the high-speed low-noise single-photon detector of gate " ultrashort pulse " (Chinese patent: 201710165360.0), use the adjustable ultrashort pulse signal of adjustable pulse width amplitude as gate-control signal, expanded using balance The working frequency of the single-photon detector of scheme, and reduce effective pulsewidth of gate signal, it can effectively reduce miscount, visited in high speed It remains to ensure that the high of spike noise inhibits ratio in survey, improves detector performance.The defect of these designs has: system described in 1. It is only used for the single-photon avalanche diode worked under gating patterns, and the single-photon detector run under gating patterns is being believed The unknown application of number photon arrival time, if luminous intensity detects, distance measurement, in laser radar and fiber optical time domain reflection instrument, The loss for be easy to causeing useful photon to count, causes system detecting error;2. system described in is only applicable to single single photon Avalanche diode is needed if required to single-photon avalanche diode array for each of array single-photon avalanche diode Related system is designed, considerably increases single-photon avalanche diode array system volume and complexity, while reducing detection The detection efficient of device system;3. the matched capacitance module of used and single-photon avalanche diode progress (or PIN photoelectricity is visited Survey device) with single-photon avalanche diode not on the same chip, when having incident light beam strikes to single-photon avalanche diode and trigger When avalanche effect, the temperature of single-photon avalanche diode can change, and internal equivalent parameters (capacitor, resistance etc.) can also become Change, will cause single-photon avalanche diode in this way can not match with equivalent modules used (capacitor or PIN photoelectric detector), Cause systematic error.
In order to solve problem above, the invention discloses one kind to be based on standard integrated circuit technology low noise single photon detection Chip and system can be used for laser radar, DNA sequencing, the detection of the poles dim light such as the distribution of quantum secret key and medical imaging.This hair It is bright in single photon detection chip by one or more single-photon avalanche diode in single-photon avalanche diode array Photosensitive part is covered with metal layer, runs it under dark situation, only provides dark counting.The single-photon avalanche run under dark situation Diode is due to the single-photon avalanche diode phase that runs under structure, size and operating parameter and normal mode on same chip Together, there can be identical dark count rate.This dark counting be used to reduce the noise of whole system, and (dark count rate theoretically can be with It drops to close to 0), for improving the sensitivity and detection dynamic range of system.Single-photon avalanche diode number of arrays on chip Amount is bigger, and the effect of noise reduction is more obvious.The single-photon avalanche diode that present invention can apply to work under any mode, including Gating patterns are passively quenched and mode are actively quenched, greatly improve its application range.The system need to only avenge single photon The a part collapsed in diode array is handled (one or more), single without carrying out to all single-photon avalanche diodes Reason of staying alone and system design, reduce system bulk and complexity, while helping to promote photon detection efficiency, this makes institute The system of stating is more suitable for single-photon detector array system.All single photons for being used to carry out single photon detection in the system Avalanche diode is on same chip, is same structure, same size and is worked under same bias voltage, therefore There are the operating temperature and performance of identical (or close), this makes its noise reduction effect will not be by single-photon detector chip temperature Variation is influenced.In addition to this, the present invention can be completed under standard integrated circuit technology (such as by the sense of single-photon avalanche diode Light part is covered with metal layer), while it being applicable to the single-photon detector array chip of different structure, this makes the present invention can To be carried out simultaneously with other optimization means such as single-photon avalanche diode structure optimizations, further to promote single-photon detection system Performance.
(3) summary of the invention
The purpose of the present invention is to provide a kind of low noise single-photon detection systems by light source 1, biasing module 2, single photon Detection chip 3, signal processing system 4 form, two pole of single-photon avalanche that wherein single photon detection chip 3 is run by normal mode Single-photon avalanche diode 32 and avalanche events detection circuit array 33 composition run under pipe 31, dark situation.
The object of the present invention is achieved like this:
Biasing module 2 generates controllable reverse bias voltage and exports to single photon detection chip 3, single photon detection chip All single-photon avalanche diodes in 3 are offset under identical voltage, and the light that light source 1 issues is incident to single photon detection core The output of single-photon avalanche diode 31 of piece 3, the normal mode operation in single photon detection chip 3 includes noise-excitation and photon Avalanche events electric pulse including excitation, and regular transistor-transistor is converted to by avalanche events detection circuit array 33 Logic level (TTL) signal is exported to signal processing system 4, and dark situation snows the single photon of operation in single photon detection chip 3 It collapses the avalanche events electric pulse of 32 output noises of diode excitation and TTL is converted to by avalanche events detection circuit array 33 Signal is exported to signal processing system 4, and signal processing system 4 carries out photon meter to the TTL signal that single photon detection chip 3 exports Digit rate calculates and noise reduction calculates and processing, finally provides detection result.
Light source 1 in the system can be the fluorescent exciting signal in fluorescence detection system, optical time domain reflection system In Ruili reflected light signal, the signal of communication in communication system, interference signal and surface in fiber optic sensor system etc. One kind of the various optical signals such as the reflection signal of ion resonance detection system.
Single photon detection chip 3 in the system is the chip based on standard integrated circuit technology, and manufacturing process can be with It is standard CMOS technique (CMOS), bipolar CMOS technique (BiCMOS), Times of silicon wafer insulator CMOS technology (SOI CMOS) and cmos image sensor technique (CIS) Anticipate one kind, process can be 0.8 μm, 0.35 μm, 0.18 μm, 0.13 μm, it is any one in 90nm, 65nm and 45nm Kind.The structure of single-photon avalanche diode in single photon detection chip 3 can by p+, the n+ in standard integrated circuit technology, The difference such as nwell, pwell, Deep-nwell, P-epitaxial and P-subtrate mix layer certain several constituted , shape can be circular, ellipse, square, one of shapes such as rectangle.
The optical detection part of single photon detection chip 3 is made of single-photon avalanche diode array, all lists in array Photon avalanches diode is on same chip, have same structure, same size and in same bias voltage and At a temperature of work.N number of single-photon avalanche diode (N >=1) is chosen in an array, with a gold in standard integrated circuit technology Belong to layer to cover photosensitive region, run it under dark situation, forms the single-photon avalanche diode run under dark situation 32, the avalanche events electric pulse of output noise excitation and to be converted to TTL signal by avalanche events detection circuit array 33 defeated Out to signal processing system 4;Remaining single-photon avalanche diode then works under normal mode, the operation of these normal modes Single-photon avalanche diode 31 exports the avalanche events electric pulse including noise-excitation and photon excitation, and passes through snowslide Event detection circuit array 33 is converted to TTL signal and exports to signal processing system 4.Snowslide thing in single photon detection chip 3 Part detection circuit array 33 can be amplitude discriminator circuit, current-to-voltage converting circuit, voltage comparator circuit and quenching circuit It is any.
The signal processing system 4 can be based on microcontroller, field programmable gate array (FPGA) and Any one of the signal processing system of computer.Signal processing system 4 receives snowslide event detection in single photon detection chip 3 The TTL signal that gate array 33 exports obtains the single-photon avalanche diode 31 of normal mode operation and dark by calculating respectively The pulsimeter digit rate that the single-photon avalanche diode 32 run under environment is exported.The single photon snow of all normal mode operations The average counter rate for collapsing diode 31 removes the average counter rate of the single-photon avalanche diode 32 run under all dark situations, then Number multiplied by the single-photon avalanche diode 31 of normal mode operation is then output of the whole detection system after removing noise Photon count rate.If the number for the single-photon avalanche diode 3 that normal mode is run in single photon detection chip 3 is M, Mei Gedan It is respectively CR that photon avalanches diode, which exports pulsimeter digit rate to be,1、CR2、CR3...CRM, the single-photon avalanche that runs under dark situation The number of diode 32 is N, and each step-by-step counting is CRD1、CRD2、 CRD3...CRDN, then whole single-photon detection system The output photon counting rate (CR) after removing noise are as follows:
(4) Detailed description of the invention
Fig. 1 is based on the low noise single photon detection chip of standard integrated circuit technology and its structural schematic diagram of system. Low noise single-photon detection system is made of light source 1, biasing module 2, single photon detection chip 3, signal processing system 4, wherein The single-photon avalanche two run under single-photon avalanche diode 31 that single photon detection chip 3 is run by normal mode, dark situation Pole pipe 32 and avalanche events detection circuit array 33 form.
Fig. 2 is showing for the embodiment one of low noise single photon detection chip and its system based on standard integrated circuit technology It is intended to.Low noise single-photon detection system is made of light source 1, biasing module 2, single photon detection chip 3, signal processing system 4, Single-photon avalanche diode 31 that wherein single photon detection chip 3 is run by normal mode, dark situation snow the single photon of operation It collapses diode 32 and avalanche events detection circuit array 33 forms.In system the optical detection part of single photon detection chip 3 by One 1 × 6 single-photon avalanche diode array is constituted, and it is integrated with standard to choose 1 single-photon avalanche diode in an array A metal layer in circuit technology is covered, and runs it under dark situation, is formed dark situation and is snowed the single photon of operation Diode 32 is collapsed, the avalanche events electric pulse of output noise excitation is simultaneously converted to by avalanche events detection circuit array 33 TTL signal is exported to signal processing system 4;Remaining single-photon avalanche diode then works under normal mode, these are normal The single-photon avalanche diode 31 of mode operation exports the avalanche events electric pulse including noise-excitation and photon excitation, and TTL signal is converted to by avalanche events detection circuit array 33 to export to signal processing system 4.
Fig. 3 is the single-photon avalanche diode run under the single-photon avalanche diode and dark situation that normal mode is run Structural schematic diagram under standard integrated circuit technology.The PN junction (avalanche multiplication area) of single-photon avalanche diode is formed in p+ floor Pwell is injected and between nwell layers, in structure around the region p+ to form a lower guarantor mixed around multiplication regions Retaining ring is isolated high electric field.The photosensitive region of the single-photon avalanche diode 32 run under dark situation has one layer of metal Layer covering (metal3) runs on it in dark situation, will not generate the avalanche events excited by absorption photon, only exports dark It counts.By the statistics to dark counting, for reducing detection system noise.
Fig. 4 is showing for the embodiment one of low noise single photon detection chip and its system based on standard integrated circuit technology It is intended to.Low noise single-photon detection system is made of light source 1, biasing module 2, single photon detection chip 3, signal processing system 4, Single-photon avalanche diode 31 that wherein single photon detection chip 3 is run by normal mode, dark situation snow the single photon of operation It collapses diode 32 and avalanche events detection circuit array 33 forms.In system the optical detection part of single photon detection chip 3 by One 1 × 10 single-photon avalanche diode array is constituted, and 10 single-photon avalanche diodes in array are in same core On piece is same structure, same size and same bias voltage and at a temperature of work.3 lists are chosen in an array Photon avalanches diode is covered with a metal layer in standard integrated circuit technology, runs it under dark situation, shape At the single-photon avalanche diode 32 run under dark situation, the avalanche events electric pulse of output noise excitation simultaneously passes through snowslide thing Part detection circuit array 33 is converted to TTL signal and exports to signal processing system 4;Remaining single-photon avalanche diode then works Under normal mode, the output of single-photon avalanche diode 31 of these normal modes operation includes noise-excitation and photon excitation Avalanche events electric pulse inside, and TTL signal is converted to by avalanche events detection circuit array 33 and is exported to signal processing System 4.
(5) specific embodiment
Below with reference to specific embodiment, the present invention is further explained.
Embodiment one:
Fig. 2 gives based on the low noise single photon detection chip of standard integrated circuit technology and its embodiment of system. Low noise single-photon detection system is made of light source 1, biasing module 2, single photon detection chip 3, signal processing system 4, wherein The single-photon avalanche two run under single-photon avalanche diode 31 that single photon detection chip 3 is run by normal mode, dark situation Pole pipe 32 and avalanche events detection circuit array 33 form.Biasing module 2 generates controllable reverse bias voltage and exports extremely Single photon detection chip 3, all single-photon avalanche diodes in single photon detection chip 3 are offset under identical voltage, The light that light source 1 issues is incident to single photon detection chip 3, the single photon snow of the normal mode operation in single photon detection chip 3 Avalanche events electric pulse of the output of diode 31 including noise-excitation and photon excitation is collapsed, and passes through avalanche events and detects electricity Road array 33 is converted to regular transistor-transistor logic level (TTL) signal and exports to signal processing system 4, single-photon detecting It surveys the avalanche events electric pulse of 32 output noises of the single-photon avalanche diode excitation run under dark situation in chip 3 and passes through Avalanche events detection circuit array 33 is converted to TTL signal and exports to signal processing system 4, and signal processing system 4 is to single photon The calibration pulse that detection chip 3 exports carries out photon count rate and noise reduction calculates and processing, finally provides detection result.
The optical detection part of single photon detection chip 3 is made of one 1 × 6 single-photon avalanche diode array, array In 6 single-photon avalanche diodes be on same chip, be same structure, same size and in same biased electrical Pressure and at a temperature of work.A gold of 1 single-photon avalanche diode in standard integrated circuit technology is chosen in an array Belong to layer to be covered, run it under dark situation, forms the single-photon avalanche diode 32 run under dark situation, only output is made an uproar The avalanche events electric pulse of sound excitation is simultaneously converted to TTL signal and is exported to signal processing by avalanche events detection circuit array 33 System 4;Remaining single-photon avalanche diode then works under normal mode, the single-photon avalanche two of these normal modes operation Pole pipe 31 exports the avalanche events electric pulse including noise-excitation and photon excitation, and passes through avalanche events detection circuit battle array Column 33 are converted to TTL signal and export to signal processing system 4.
The single-photon avalanche diode 32 run under the single-photon avalanche diode 31 and dark situation of normal mode operation Structure under standard integrated circuit technology is as shown in Figure 3.The PN knot (avalanche multiplication area) of single-photon avalanche diode is formed in Pwell is injected between p+ layers and nwell layers, in structure around the region p+ to form a lower ginseng around multiplication regions High electric field is isolated in miscellaneous protection ring.The photosensitive region of the single-photon avalanche diode 32 run under dark situation has one Layer metal layer covering (Metal3) runs on it in dark situation, will not generate the avalanche events excited by absorption photon, only Export dark counting.By the statistics to dark counting, for reducing detection system noise.
Signal processing system 4 receives the TTL letter that snowslide event detection circuit array 33 exports in single photon detection chip 3 Number, and by calculating the single photon run under the single-photon avalanche diode 31 and dark situation that obtain normal mode operation respectively The pulsimeter digit rate that avalanche diode 32 is exported.The single-photon avalanche diode output of 5 normal mode operations in array Pulsimeter digit rate is respectively CR1, CR2, CR3, CR4 and CR5, the single-photon avalanche diode output run under 1 dark situation Pulsimeter digit rate is CRD1.Overall output photon count rate (CR after the noise reduction that signal processing system 4 obtainss) are as follows:
Embodiment two:
Fig. 4 gives based on the low noise single photon detection chip of standard integrated circuit technology and its embodiment of system. Low noise single-photon detection system is made of light source 1, biasing module 2, single photon detection chip 3, signal processing system 4, wherein The single-photon avalanche two run under single-photon avalanche diode 31 that single photon detection chip 3 is run by normal mode, dark situation Pole pipe 32 and avalanche events detection circuit array 33 form.Biasing module 2 generates controllable reverse bias voltage and exports extremely Single photon detection chip 3, all single-photon avalanche diodes in single photon detection chip 3 are offset under identical voltage, The light that light source 1 issues is incident to single photon detection chip 3, the single photon snow of the normal mode operation in single photon detection chip 3 Avalanche events electric pulse of the output of diode 31 including noise-excitation and photon excitation is collapsed, and passes through avalanche events and detects electricity Road array 33 is converted to regular transistor-transistor logic level (TTL) signal and exports to signal processing system 4, single-photon detecting It surveys the avalanche events electric pulse of 32 output noises of the single-photon avalanche diode excitation run under dark situation in chip 3 and passes through Avalanche events detection circuit array 33 is converted to TTL signal and exports to signal processing system 4, and signal processing system 4 is to single photon The calibration pulse that detection chip 3 exports carries out photon count rate and noise reduction calculates and processing, finally provides detection result.
The optical detection part of single photon detection chip 3 is made of one 1 × 10 single-photon avalanche diode array, array In 10 single-photon avalanche diodes be on same chip, be same structure, same size and similarly biasing Voltage and at a temperature of work.3 single-photon avalanche diodes are chosen in an array with one in standard integrated circuit technology Metal layer is covered, and runs it under dark situation, is formed the single-photon avalanche diode 32 run under dark situation, is only exported The avalanche events electric pulse of noise-excitation is simultaneously converted to TTL signal and is exported to signal by avalanche events detection circuit array 33 Reason system 4;Remaining single-photon avalanche diode then works under normal mode, the single-photon avalanche of these normal modes operation Diode 31 exports the avalanche events electric pulse including noise-excitation and photon excitation, and passes through avalanche events detection circuit Array 33 is converted to TTL signal and exports to signal processing system 4.
Signal processing system 4 receives the TTL letter that snowslide event detection circuit array 33 exports in single photon detection chip 3 Number, and by calculating the single photon run under the single-photon avalanche diode 31 and dark situation that obtain normal mode operation respectively The pulsimeter digit rate that avalanche diode 32 is exported.The single-photon avalanche diode output of 7 normal mode operations in array Pulsimeter digit rate is respectively CR1, CR2, CR3, CR4, CR5, CR6 and CR7, two pole of single-photon avalanche run under 3 dark situations The pulsimeter digit rate of pipe output is CRD1, CRD2And CRD3.Overall output after the noise reduction that signal processing system 4 obtains Photon count rate (CRs) are as follows:

Claims (4)

1. one kind is based on standard integrated circuit technology low noise single photon detection chip and system.It is characterized in that: low noise monochromatic light Sub- detection system is made of light source 1, biasing module 2, single photon detection chip 3, signal processing system 4, wherein single photon detection The single-photon avalanche diode 32 that is run under single-photon avalanche diode 31 that chip 3 is run by normal mode, dark situation and Avalanche events detection circuit array 33 forms.Biasing module 2 generates controllable reverse bias voltage and exports extremely in the system Single photon detection chip 3, all single-photon avalanche diodes in single photon detection chip 3 are offset under identical voltage, The light that light source 1 issues is incident to single photon detection chip 3, the single photon snow of the normal mode operation in single photon detection chip 3 Avalanche events electric pulse of the output of diode 31 including noise-excitation and photon excitation is collapsed, and passes through avalanche events and detects electricity Road array 33 is converted to regular transistor-transistor logic level (TTL) signal and exports to signal processing system 4, single-photon detecting It surveys the avalanche events electric pulse of 32 output noises of the single-photon avalanche diode excitation run under dark situation in chip 3 and passes through Avalanche events detection circuit array 33 is converted to TTL signal and exports to signal processing system 4, and signal processing system 4 is to single photon The TTL signal that detection chip 3 exports carries out photon count rate calculating and noise reduction calculates and processing, finally provides detection result.
2. light source 1 according to claim 1.It is characterized in that: the light source 1 in the system can be in fluorescence detection system Fluorescent exciting signal, the Ruili reflected light signal in optical time domain reflection system, the signal of communication in communication system, optical fiber passes One kind of the various optical signals such as the reflection signal of interference signal and surface plasma resonance detection system in sensor system.
3. single photon detection chip 3 according to claim 1 and its system.It is characterized in that: the single photon detection chip 3 is Based on the chip of standard integrated circuit technology, manufacturing process can be standard CMOS technique (CMOS), Bipolar CMOS technique (BiCMOS), silicon wafer insulator CMOS technology (SOI CMOS) and cmos image sensor technique (CIS) any one, process can be 0.8 μm, 0.35 μm, 0.18 μm, 0.13 μm, any one in 90nm, 65nm and 45nm.The optical detection part of single photon detection chip 3 is by single-photon avalanche Diode array is constituted, and all single-photon avalanche diodes are on same chip in array, there is same structure, same Size and same bias voltage and at a temperature of work.N number of single-photon avalanche diode (N >=1) is chosen in an array, Photosensitive region is covered with a metal layer in standard integrated circuit technology, runs it under dark situation, is formed dark The single-photon avalanche diode 32 run under environment, the avalanche events electric pulse of output noise excitation are simultaneously examined by avalanche events Slowdown monitoring circuit array 33 is converted to TTL signal and exports to signal processing system 4;Remaining single-photon avalanche diode then works in just Under norm formula, the single-photon avalanche diode 31 of these normal modes operation is exported including noise-excitation and photon excitation Avalanche events electric pulse, and TTL signal is converted to by avalanche events detection circuit array 33 and is exported to signal processing system 4. Avalanche events detection circuit array 33 in single photon detection chip 3 can be amplitude discriminator circuit, current-to-voltage converting circuit, electricity Press any one of comparison circuit and quenching circuit.
4. signal processing system 4 according to claim 1.It is characterized in that: the signal processing system 4 can be and be based on Any one of the signal processing system of microcontroller, field programmable gate array (FPGA) and computer.At signal Reason system 4 receives the TTL signal that snowslide event detection circuit array 33 exports in single photon detection chip 3, distinguishes by calculating Show that the single-photon avalanche diode 32 run under the single-photon avalanche diode 31 and dark situation of normal mode operation is exported Pulsimeter digit rate.The average counter rate of the single-photon avalanche diode 31 of all normal mode operations removes all dark situations The average counter rate of the single-photon avalanche diode 32 of lower operation, multiplied by the single-photon avalanche diode 31 run in the normal mode Number be then output photon counting rate of the whole detection system after removing noise.
CN201811182461.XA 2018-10-11 2018-10-11 Low-noise single photon detection chip and system based on standard integrated circuit process Active CN109253807B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201811182461.XA CN109253807B (en) 2018-10-11 2018-10-11 Low-noise single photon detection chip and system based on standard integrated circuit process

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201811182461.XA CN109253807B (en) 2018-10-11 2018-10-11 Low-noise single photon detection chip and system based on standard integrated circuit process

Publications (2)

Publication Number Publication Date
CN109253807A true CN109253807A (en) 2019-01-22
CN109253807B CN109253807B (en) 2020-10-13

Family

ID=65045088

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201811182461.XA Active CN109253807B (en) 2018-10-11 2018-10-11 Low-noise single photon detection chip and system based on standard integrated circuit process

Country Status (1)

Country Link
CN (1) CN109253807B (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2576607A (en) * 2019-06-26 2020-02-26 X Fab Semiconductor Foundries Gmbh Single photon avalanche diode devices
CN111121986A (en) * 2019-12-25 2020-05-08 桂林电子科技大学 Single photon detection system with rear pulse correction function

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101545810A (en) * 2008-03-26 2009-09-30 中国科学技术大学 High-speed single photon detection method and detector
CN201497580U (en) * 2009-09-21 2010-06-02 安徽问天量子科技股份有限公司 GHz pulse door control low-pass filter infrared single-photon detector
CN102155998A (en) * 2011-04-01 2011-08-17 张军 Fully-integrated high-speed single photon detecting system and detecting method
CN102820365A (en) * 2012-08-22 2012-12-12 上海交通大学 Semiconductor infrared up-conversion single photon detection equipment and method
CN203191082U (en) * 2013-04-09 2013-09-11 桂林电子科技大学 Back-end acquisition card for photon counter module
US20160291138A1 (en) * 2015-04-02 2016-10-06 Stmicroelectronics (Grenoble 2) Sas Wrap around ranging method and circuit
CN107036722A (en) * 2017-03-31 2017-08-11 上海理工大学 The high-speed low-noise single-photon detection system of ultrashort pulse gate
CN107271055A (en) * 2016-04-20 2017-10-20 中国科学技术大学 A kind of infrared single photon detectorses system of parallel avalanche photodiode array structure
JP2018009903A (en) * 2016-07-14 2018-01-18 シャープ株式会社 Fluorescence inspection system

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101545810A (en) * 2008-03-26 2009-09-30 中国科学技术大学 High-speed single photon detection method and detector
CN201497580U (en) * 2009-09-21 2010-06-02 安徽问天量子科技股份有限公司 GHz pulse door control low-pass filter infrared single-photon detector
CN102155998A (en) * 2011-04-01 2011-08-17 张军 Fully-integrated high-speed single photon detecting system and detecting method
CN102820365A (en) * 2012-08-22 2012-12-12 上海交通大学 Semiconductor infrared up-conversion single photon detection equipment and method
CN203191082U (en) * 2013-04-09 2013-09-11 桂林电子科技大学 Back-end acquisition card for photon counter module
US20160291138A1 (en) * 2015-04-02 2016-10-06 Stmicroelectronics (Grenoble 2) Sas Wrap around ranging method and circuit
CN107271055A (en) * 2016-04-20 2017-10-20 中国科学技术大学 A kind of infrared single photon detectorses system of parallel avalanche photodiode array structure
JP2018009903A (en) * 2016-07-14 2018-01-18 シャープ株式会社 Fluorescence inspection system
CN107036722A (en) * 2017-03-31 2017-08-11 上海理工大学 The high-speed low-noise single-photon detection system of ultrashort pulse gate

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2576607A (en) * 2019-06-26 2020-02-26 X Fab Semiconductor Foundries Gmbh Single photon avalanche diode devices
GB2576607B (en) * 2019-06-26 2021-06-16 X Fab Semiconductor Foundries Gmbh Single photon avalanche diode devices
US11575061B2 (en) 2019-06-26 2023-02-07 X-Fab Semiconductor Foundries Gmbh Single photon avalanche diode devices
CN111121986A (en) * 2019-12-25 2020-05-08 桂林电子科技大学 Single photon detection system with rear pulse correction function

Also Published As

Publication number Publication date
CN109253807B (en) 2020-10-13

Similar Documents

Publication Publication Date Title
Palubiak et al. CMOS SPADs: Design issues and research challenges for detectors, circuits, and arrays
Piemonte et al. Overview on the main parameters and technology of modern Silicon Photomultipliers
Sanzaro et al. Single-photon avalanche diodes in a 0.16 μm BCD technology with sharp timing response and red-enhanced sensitivity
Zappa et al. Solid-state single-photon detectors
Niclass et al. A single photon avalanche diode implemented in 130-nm CMOS technology
Cova et al. Evolution and prospects for single-photon avalanche diodes and quenching circuits
Bronzi et al. Low-noise and large-area CMOS SPADs with timing response free from slow tails
KR20210068585A (en) High Quantum Efficiency Geiger Mode Avalanche Diodes Containing High Sensitivity Photon Mixing Structures and Arrays Thereof
CN108231947B (en) Single photon avalanche diode detector structure and manufacturing method thereof
Sun et al. A simple analytic modeling method for SPAD timing jitter prediction
CN109459149A (en) A kind of measurement of high-precision single photon detection chip real time temperature and performance optimization system
Vornicu et al. Design of high-efficiency SPADs for LiDAR applications in 110nm CIS technology
WO2012063027A2 (en) Photon detector
CN109253807A (en) Based on standard integrated circuit technology low noise single photon detection chip and system
Wang et al. Design and measurement of ring-gate single photon avalanche diode with low dark count rate
Korpar Status and perspectives of solid state photon detectors
US11978754B2 (en) High quantum efficiency Geiger-mode avalanche diodes including high sensitivity photon mixing structures and arrays thereof
Dinu Silicon photomultipliers (SiPM)
Liu et al. Accurate prediction of photon detection probability based on the 2-D dead-space model for SPADs
D’Ascenzo et al. Design and Characterization of a Silicon Photomultiplier in 0.35-${\mu}\text {m} $ CMOS
Saveliev Silicon photomultiplier-new era of photon detection
Deng et al. Design and analysis of a photon counting system using covered single-photon avalanche photodiode
Yue et al. Performance of ultra-small silicon photomultiplier array with active area of 0.12 mm× 0.12 mm
Wang et al. Electric-field-drive single photon avalanche diode with barrier enhancement for fluorescence detection
Charbon et al. SPAD sensors come of age

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
TA01 Transfer of patent application right
TA01 Transfer of patent application right

Effective date of registration: 20200817

Address after: No.1 building, No.333, Haiyang 1st Road, Lingang New Area, China (Shanghai) pilot Free Trade Zone, Pudong New Area, Shanghai, 201306

Applicant after: Chuanzhou semiconductor technology (Shanghai) Co.,Ltd.

Address before: 541004 Guilin Guilin, 1 Jinji Road, Guilin, the Guangxi Zhuang Autonomous Region

Applicant before: GUILIN University OF ELECTRONIC TECHNOLOGY

GR01 Patent grant
GR01 Patent grant
PE01 Entry into force of the registration of the contract for pledge of patent right
PE01 Entry into force of the registration of the contract for pledge of patent right

Denomination of invention: Low noise single photon detection chip and system based on standard integrated circuit technology

Effective date of registration: 20231102

Granted publication date: 20201013

Pledgee: Industrial Commercial Bank of China Ltd. Shanghai Zhangjiang science and Technology Branch

Pledgor: Chuanzhou semiconductor technology (Shanghai) Co.,Ltd.

Registration number: Y2023980063923