CN106482829A - The dynamic and static combined test system of single-photon detector and its method of testing - Google Patents

The dynamic and static combined test system of single-photon detector and its method of testing Download PDF

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Publication number
CN106482829A
CN106482829A CN201610836161.3A CN201610836161A CN106482829A CN 106482829 A CN106482829 A CN 106482829A CN 201610836161 A CN201610836161 A CN 201610836161A CN 106482829 A CN106482829 A CN 106482829A
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dark current
dark
current
snowslide
afterpulse
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CN106482829B (en
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连洁
王莹
李永富
刘俊良
张庭发
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Shandong University
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Shandong University
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/42Photometry, e.g. photographic exposure meter using electric radiation detectors
    • G01J1/44Electric circuits
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/42Photometry, e.g. photographic exposure meter using electric radiation detectors
    • G01J1/44Electric circuits
    • G01J2001/444Compensating; Calibrating, e.g. dark current, temperature drift, noise reduction or baseline correction; Adjusting
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J1/00Photometry, e.g. photographic exposure meter
    • G01J1/42Photometry, e.g. photographic exposure meter using electric radiation detectors
    • G01J1/44Electric circuits
    • G01J2001/4446Type of detector
    • G01J2001/446Photodiode
    • G01J2001/4466Avalanche

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

Abstract

The invention discloses a kind of dynamic and static combined test system of single-photon detector, including digital sourcemeter, changing device, test circuit and oscillograph, avalanche diode is positioned in the incubation chamber in changing device, the negative electrode of avalanche diode is connected with the outfan of digital sourcemeter, the anode of avalanche diode is connected with the input of test circuit, the output waveform of avalanche diode connects to oscillographic input, and the outfan of test circuit connects to computer.Due to different temperatures, different overbias and under the different dead time, the composition of dark current can change, and the present invention joins together to be separated by dynamic test and static test it is achieved that dynamically debugging in real time in combination with static state;And determine the composition of dark current, and this determines that the method that dark current is constituted easily is realized, therefore, dark current is constituted not only goes up Theoretical Calculation, experimentally also easily proves.

Description

The dynamic and static combined test system of single-photon detector and its method of testing
Technical field
The present invention relates to a kind of dynamic and static combined test system of single-photon detector and its method of testing, belong to micro- Optical detector technology field.
Background technology
Single-photon detecting survey technology, is the powerful measure of detection faint optical signal, has extensively in quantum communications, laser ranging etc. General application.The principal element limiting single-photon detector quantum efficiency at present is dark counting and afterpulse, is to lead to quantum to lead to The key factor of the bit error rate in letter.Photoelectric detector (as avalanche photodide) is an important set of single-photon detector Become part, be dark current respectively and be captured releasing again of carrier with detector dark counting, the corresponding parameter of afterpulse probability Put the electric current of generation, therefore, in order to reduce the dark counting of single-photon detector and afterpulse probability it is necessary to analyze avalanche diode The source of dark current, research reduces dark current, the method for afterpulse effect, could improve the performance of single-photon detector.Work The noise of the single-photon detector under Geiger mode angular position digitizer is mainly derived from three classes:Random noise that thermal noise causes, high-V alloy It is afterpulse effect that lower carrier occurs tunneling effect to cause snowslide, trapping centre to discharge carrier again.Afterpulse effect is in reality Test be relatively easy to distinguish, although and thermal noise and tunnelling current have the strict derivation of equation in theory, experimentally divide Do not obtain still more difficult.The composition determining dark current is also one study hotspot of monochromatic light subdomains instantly.
Avalanche diode is a kind of high diode of sensitivity, and slightly larger electric current can be to be allowed to damage, therefore right When it is tested certain it is noted that restriction to electric current.In existing static test, its I-V, C-V curve need by means of half Conductor parameter analyzer, but do not enable real-time control;Can also be by digital sourcemeter, it is possible to achieve real-time control, but C-V curve can not be obtained.And the control for temperature needs by means of becoming circuit temperature, mainly adopt semiconductor refrigerating, system at present Speed of cooling is fast and low cost.Single-photon detector photoelectric detector (as avalanche photodide) generally to be comprised, device drive Galvanic electricity road and output signal extract circuit, and the test to the dark counting of its whole system etc. is referred to as dynamic test.And for same For the avalanche diode of sample, static and dynamically to test the result obtaining be different, static test can obtain total Dark current, and dynamic test can obtain dark counting feature.And static test system and dynamic test system are for a lot of parameters Definition mode have bigger difference, such as avalanche breakdown voltage.In static test, avalanche breakdown voltage is that snow dark current reaches certain Bias voltage value during one value;And in dynamic circuit, occur more than bias voltage value during a certain output pulse for first time. Fact proved, both is widely different.Therefore, it is necessary to joint test, to realize the purpose of efficient accurate measurement.
Content of the invention
The present invention is in order to overcome the shortcomings of above technology, there is provided a kind of dynamic and static state of single-photon detector combines survey Test system and its method of testing, dynamic test and static test are succinctly efficiently combined by this method of testing is tested, Achieve dynamic and static unified debugging, to reach the purpose determining that dark current is constituted.
The present invention overcomes its technical problem be employed technical scheme comprise that:
A kind of dynamic and static combined test system of single-photon detector, including digital sourcemeter, changing device, test electricity Road and oscillograph, avalanche diode is positioned in the incubation chamber in changing device, the negative electrode of avalanche diode and digital sourcemeter Outfan connects, the anode of avalanche diode is connected with the input of test circuit, the output waveform of avalanche diode connect to Oscillographic input, the outfan of test circuit connects to computer.
According to currently preferred, digital sourcemeter adopts Keithley 2400 digital sourcemeter.
Present invention also offers a kind of test of the dynamic and static combined test system using above-mentioned single-photon detector Method, step is as follows:
S1, fix a temperature value, this temperature span is -50 DEG C~20 DEG C, digital sourcemeter to avalanche diode plus Bias, observes the dark counting of the electric current registration, oscilloscope display waveform and computer acquisition on digital sourcemeter;
S2, it is gradually increased and is biased into avalanche breakdown voltage, at this moment on digital sourcemeter, the electric current of display becomes larger, and shows simultaneously On ripple device, the waveform of display starts snowslide pulse, and non-zero numeral also in dark counting;Under avalanche breakdown voltage state, number On the table of word source, the electric current of display is total dark current Idark, on oscillograph, the avalanche voltage waveform of appearance is calculated by Ohm's law Obtain corresponding current value, current curve be integrated, obtain single snowslide quantity of electric charge Q,
Wherein, T1Represent the moment shown by oscillograph, T when avalanche signal starts to occur2Represent avalanche signal will disappear When shown moment;
S3, obtain the numerical value n of dark counting from test circuit, then obtain total snowslide quantity of electric charge QaFor the single snowslide quantity of electric charge The product of Q and dark count numerical value n, and then obtain snowslide dark current Ia,
That is, IaIt is the dark current sum being caused with afterpulse due to the dark current that thermal noise and tunneling effect cause, wherein, τ is the dead time;
S4, determine the composition of dark current and the test of dark current:Have neither part nor lot in the dark current I of snowslidebMainly leaked by surface Electric current causes, snowslide dark current IaThe main dark current I being caused by thermal noiseth, the dark current I that causes of tunneling effectTATAnd after The dark current I that pulse causescConstitute;
S4.1, have neither part nor lot in the dark current I of snowslideb
Total dark current IdarkDeduct snowslide dark current IaAs have neither part nor lot in the dark current I of snowslideb
The dark current I that S4.2, thermal noise causeth
In the case that barrier width is constant, penetration coefficient is relevant with depletion region electric field, the dark electricity that is, tunneling effect causes Stream ITATOnly relevant with overbias, and afterpulse can be adjusted by dead time τ, as τ >=20 μ s, afterpulse can be ignored, because This, can be by the dead time τ, the dark current I that tunneling effect causes of fixing overbias and setting >=20 μ sTATIn snowslide dark current IaIn numerical value be fixing, the dark current I that afterpulse causescNegligible, and then can be from IaIn isolate Ith:Fixing Overbias and the dead time τ of setting >=20 μ s, constantly reduce temperature, obtain the dark counting under different temperatures, obtain dark after matching Count the relation curve with temperature T, I be can get by dark countingaValue, and then I can be obtainedaWith the relation curve of temperature T, Represent the I under different temperaturesaDifference be the change of the lower thermal noise of relevant temperature change, then with thermal noise curve in theoryIt is compared;
The dark current I that S4.3, tunneling effect causeTAT
When temperature≤- 40 DEG C, the dark current I that thermal noise leads tothCan ignore, at this moment can obtain tunneling effect and cause Dark current ITATAnd the dark current I that afterpulse causesc;In temperature≤- 20 DEG C, overbias >=3V, increase dead time τ extremely >=20 μ s, can ignore the electric current that afterpulse causes, you can separate and obtain the dark current I that tunneling effect causesTAT
The dark current I that S4.4, afterpulse causec
According to the measurement result of step S4.2 and S4.3, by snowslide dark current IaDeduct the dark current I that thermal noise leads toth The dark current I causing with tunneling effectTAT, obtain the dark current I that afterpulse causesc.
According to currently preferred, in described step S4.2, if the actual measurement thermal noise curve obtaining is bent with theoretical thermal noise The trend of line is identical and numerical value difference is in allowed band, then illustrate that this experimental result is correct;If numerical value difference exceedes permission model Enclose, then continue to increase the dead time, reduce temperature, then be compared, until obtaining the result in allowed band.
The invention has the beneficial effects as follows:
Due to different temperatures, different overbias and under the different dead time, the composition of dark current can change, and the present invention passes through A kind of simple method (i.e. dynamic test and static test are joined together) is separated it is achieved that dynamic and static state reality in combination When debugging;And determine the composition of dark current, and this determines that the method that dark current is constituted easily is realized, therefore, dark current is constituted Not only go up Theoretical Calculation, experimentally also easily prove.
Brief description
Fig. 1 is the structural representation of the test system of the present invention.In figure, 1, digital sourcemeter;2nd, changing device;3rd, test electricity Road;4th, oscillograph;5th, computer.
Fig. 2 is 0.2V for overbias, through 100 times of avalanche signal curve charts obtaining from oscillograph after amplifying.In figure, indulges Coordinate is voltage, and every lattice represent 20mV;Abscissa is the time, and every lattice represent 50ns.
The graph of relation that Fig. 3 is dark counting and temperature T in the case of 1.5V, 2.0V, 2.5V, 3.0V for overbias.In figure, Vertical coordinate is dark counting;Abscissa is temperature.
Specific embodiment
It is better understood from the present invention for the ease of those skilled in the art, with specific embodiment, the present invention is done below in conjunction with the accompanying drawings Further describe, following is only exemplary not limit protection scope of the present invention.
Embodiment 1,
The dynamic and static combined test system of single-photon detector of the present invention, as shown in figure 1, include digital source Table 1, changing device 2, test circuit 3 and oscillograph 4, digital sourcemeter 1 adopts Keithley 2400 digital sourcemeter, and oscillograph 4 is not Need, using more expensive current probe, directly voltage to be tested, oscillograph has the impedance matching of 50 Ω it is easy to by ohm Law obtains curent change, and digital sourcemeter 1 can also can obtain the device of electric current by arranging voltage with other;Snowslide two pole Pipe is positioned in the incubation chamber in changing device 2, and the negative electrode of avalanche diode is connected with the outfan of digital sourcemeter 1, snowslide two The anode of pole pipe is connected with the input of test circuit 3, and the output waveform of avalanche diode connects to the input of oscillograph 4, The outfan of test circuit 3 is connected to computer 5 by USB.
Embodiment 2,
A kind of method of testing of the dynamic and static combined test system of the single-photon detector described in utilization embodiment 1, Step is as follows:
S1, fix a temperature value, this temperature span is -50 DEG C~20 DEG C, digital sourcemeter to avalanche diode plus Bias, observes the dark counting of the electric current registration, oscilloscope display waveform and computer acquisition on digital sourcemeter.
S2, it is gradually increased and is biased into avalanche breakdown voltage, at this moment on digital sourcemeter, the electric current of display becomes larger (pA-nA- μ A), on oscillograph, the waveform of display starts snowslide pulse, as shown in Fig. 2 non-zero numeral also in dark counting simultaneously;Snow Collapse under breakdown voltage state, on digital sourcemeter, the electric current of display is total dark current Idark, the avalanche voltage of appearance on oscillograph Waveform is calculated corresponding current value by Ohm's law, and current curve is integrated, and obtains the single snowslide quantity of electric charge Q,
Wherein, T1Represent the moment shown by oscillograph, T when avalanche signal starts to occur2Represent avalanche signal will disappear When shown moment.
S3, obtain the numerical value n of dark counting from test circuit, then obtain total snowslide quantity of electric charge QaFor the single snowslide quantity of electric charge The product of Q and dark count numerical value n, and then obtain snowslide dark current Ia,
That is, IaIt is the dark current sum being caused with afterpulse due to the dark current that thermal noise and tunneling effect cause, wherein, τ is the dead time.
S4, after above-mentioned steps S1, S2 and S3, it is then determined that the test of the composition of dark current and dark current:Do not join Dark current I with snowslidebMainly caused by tracking current, snowslide dark current IaThe main dark current I being caused by thermal noiseth、 The dark current I that tunneling effect causesTATAnd the dark current I that afterpulse causescConstitute.
S4.1, have neither part nor lot in the dark current I of snowslideb
Total dark current IdarkDeduct snowslide dark current IaAs have neither part nor lot in the dark current I of snowslideb.
The dark current I that S4.2, thermal noise causeth
In the case that barrier width is constant, penetration coefficient is relevant with depletion region electric field, the dark electricity that is, tunneling effect causes Stream ITATOnly relevant with overbias, and afterpulse can be adjusted by dead time τ, in the case that the dead time is larger, the present embodiment selects When taking τ >=20 μ s, afterpulse can be ignored, and therefore, can be imitated by the dead time τ of fixing overbias and setting >=20 μ s, tunnelling The dark current I that should causeTATIn snowslide dark current IaIn numerical value be fixing, the dark current I that afterpulse causescNegligible not Meter, and then can be from IaIn isolate Ith:Fixing overbias and the dead time τ of setting >=20 μ s, constantly reduce temperature, obtain not Dark counting under synthermal, obtains the relation curve of dark counting and temperature T after matching, as shown in figure 3, as can be seen from Figure 3, no Under same overbias, the rising dark counting with temperature all increases, and the increase with overbias, and dark counting also increases;Then I be can get by dark countingaValue, the therefore relation curve of dark counting and temperature T passes through vertical coordinate and converts to obtain IaWith temperature The relation curve of degree T, represents the I under different temperaturesaDifference be the change of the lower thermal noise of relevant temperature change, then with reason By upper thermal noise curveIt is compared;If the actual measurement thermal noise curve obtaining is become with theoretical thermal noise curve Gesture is identical and numerical value difference is in allowed band, then illustrate that this experimental result is correct;If numerical value difference exceedes allowed band, continue Continuous increase dead time, reduction temperature, reduce temperature and can be selected for sterlin refrigerator, then be compared, until obtaining allowing model Result in enclosing.
The dark current I that S4.3, tunneling effect causeTAT
When temperature is especially low, the present embodiment chooses temperature≤- 40 DEG C, the dark current I that thermal noise leads tothCan ignore, At this moment the dark current I that tunneling effect causes can be obtainedTATAnd the dark current I that afterpulse causesc;In temperature≤- 20 DEG C, mistake During bias >=3V, increase dead time τ to >=20 μ s, the electric current that afterpulse causes can be ignored, you can separate and obtain tunneling effect The dark current I causingTAT.
The dark current I that S4.4, afterpulse causec
According to the measurement result of step S4.2 and S4.3, by snowslide dark current IaDeduct the dark current I that thermal noise leads toth The dark current I causing with tunneling effectTAT, obtain the dark current I that afterpulse causesc.So far, obtained tracking current to cause Dark current Ib, the dark current I that causes of thermal noiseth, the dark current I that causes of tunneling effectTATAnd the dark current that afterpulse causes Ic, so that it is determined that the composition of dark current.
Above only describes ultimate principle and the preferred implementation of the present invention, those skilled in the art can be according to foregoing description Make many changes and improvements, these changes and improvements should belong to protection scope of the present invention.

Claims (4)

1. a kind of single-photon detector dynamic and static combined test system it is characterised in that:Including digital sourcemeter (1), become Warm device (2), test circuit (3) and oscillograph (4), avalanche diode is positioned in the incubation chamber in changing device (2), snowslide The negative electrode of diode is connected with the outfan of digital sourcemeter (1), the input of the anode of avalanche diode and test circuit (3) even Connect, the output waveform of avalanche diode connects to the input of oscillograph (4), and the outfan of test circuit (3) connects to calculating Machine (5).
2. test system according to claim 1 it is characterised in that:Digital sourcemeter (1) adopts Keithley2400 numeral Source table.
3. the method for testing of the dynamic and static combined test system of single-photon detector according to claim 1 and 2, its It is characterised by, as follows including step:
S1, fix a temperature value, this temperature span is -50 DEG C~20 DEG C, digital sourcemeter to avalanche diode biasing, Observe the dark counting of the electric current registration, oscilloscope display waveform and computer acquisition on digital sourcemeter;
S2, it is gradually increased and is biased into avalanche breakdown voltage, at this moment on digital sourcemeter, the electric current of display becomes larger, oscillograph simultaneously The waveform of upper display starts snowslide pulse, and non-zero numeral also in dark counting;Under avalanche breakdown voltage state, digital source On table, the electric current of display is total dark current Idark, on oscillograph, the avalanche voltage waveform of appearance is calculated by Ohm's law Corresponding current value, is integrated to current curve, obtains single snowslide quantity of electric charge Q,
Q = ∫ T 1 T 2 I ( t ) d t
Wherein, T1Represent the moment shown by oscillograph, T when avalanche signal starts to occur2Represent avalanche signal will disappear when institute The moment of display;
S3, obtain the numerical value n of dark counting from test circuit, then obtain total snowslide quantity of electric charge QaFor single snowslide quantity of electric charge Q and secretly The product of count value n, and then obtain snowslide dark current Ia,
I a = Q a T = ∫ T 1 T 2 I ( t ) d t ( T 2 - T 1 ) ( 1 - n τ )
That is, IaIt is the dark current sum being caused with afterpulse due to the dark current that thermal noise and tunneling effect cause, wherein, τ is dead Time;
S4, determine the composition of dark current and the test of dark current:Have neither part nor lot in the dark current I of snowslidebMainly drawn by tracking current Rise, snowslide dark current IaThe main dark current I being caused by thermal noiseth, the dark current I that causes of tunneling effectTATAnd afterpulse draws The dark current I risingcConstitute;
S4.1, have neither part nor lot in the dark current I of snowslideb
Total dark current IdarkDeduct snowslide dark current IaAs have neither part nor lot in the dark current I of snowslideb
The dark current I that S4.2, thermal noise causeth
In the case that barrier width is constant, penetration coefficient is relevant with depletion region electric field, the dark current I that is, tunneling effect causesTAT Only relevant with overbias, and afterpulse can be adjusted by dead time τ, as τ >=20 μ s, afterpulse can be ignored, and therefore, can lead to Cross fixing overbias and the dead time τ, the dark current I that tunneling effect causes of setting >=20 μ sTATIn snowslide dark current IaIn number Value is fixing, the dark current I that afterpulse causescNegligible, and then can be from IaIn isolate Ith:Fixing overbias and The dead time τ of setting >=20 μ s, constantly reduces temperature, obtains the dark counting under different temperatures, obtains dark counting and temperature after matching The relation curve of degree T, can get I by dark countingaValue, and then I can be obtainedaWith the relation curve of temperature T, represent difference At a temperature of IaDifference be the change of the lower thermal noise of relevant temperature change, then with thermal noise curve in theoryIt is compared;
The dark current I that S4.3, tunneling effect causeTAT
When temperature≤- 40 DEG C, the dark current I that thermal noise leads tothCan ignore, at this moment can obtain that tunneling effect causes is dark Electric current ITATAnd the dark current I that afterpulse causesc;In temperature≤- 20 DEG C, overbias >=3V, increase dead time τ to >=20 μ S, can ignore the electric current that afterpulse causes, you can separate and obtain the dark current I that tunneling effect causesTAT
The dark current I that S4.4, afterpulse causec
According to the measurement result of step S4.2 and S4.3, by snowslide dark current IaDeduct the dark current I that thermal noise leads tothAnd tunnel Wear the dark current I that effect causesTAT, obtain the dark current I that afterpulse causesc.
4. method of testing according to claim 3 is it is characterised in that in described step S4.2, if the actual measurement heat obtaining is made an uproar Acoustic curve is identical with the trend of theoretical thermal noise curve and numerical value difference is in allowed band, then illustrate that this experimental result is correct; If numerical value difference exceedes allowed band, continue to increase the dead time, reduce temperature, then be compared, until obtaining allowing model Result in enclosing.
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JP2019203736A (en) * 2018-05-22 2019-11-28 株式会社デンソー Photodetector and control method therefor
CN112763880A (en) * 2020-12-23 2021-05-07 广州广电计量检测(上海)有限公司 Repeated avalanche tolerance test system
CN113686433A (en) * 2021-08-23 2021-11-23 长飞光纤光缆股份有限公司 Photoelectric detector and erbium-doped optical fiber amplifier based on dark current compensation
CN113791755A (en) * 2021-08-24 2021-12-14 中国航天科工集团第二研究院 Quantum random number sequence generation method, system and device
CN114112030A (en) * 2021-12-06 2022-03-01 江西省纳米技术研究院 Photoelectric detector performance testing device based on artificial intelligence

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Publication number Priority date Publication date Assignee Title
JP2019203736A (en) * 2018-05-22 2019-11-28 株式会社デンソー Photodetector and control method therefor
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CN112763880A (en) * 2020-12-23 2021-05-07 广州广电计量检测(上海)有限公司 Repeated avalanche tolerance test system
CN113686433A (en) * 2021-08-23 2021-11-23 长飞光纤光缆股份有限公司 Photoelectric detector and erbium-doped optical fiber amplifier based on dark current compensation
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CN114112030A (en) * 2021-12-06 2022-03-01 江西省纳米技术研究院 Photoelectric detector performance testing device based on artificial intelligence

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