CN109557573A - A kind of digitlization α/β ray discriminating method - Google Patents

A kind of digitlization α/β ray discriminating method Download PDF

Info

Publication number
CN109557573A
CN109557573A CN201811448004.0A CN201811448004A CN109557573A CN 109557573 A CN109557573 A CN 109557573A CN 201811448004 A CN201811448004 A CN 201811448004A CN 109557573 A CN109557573 A CN 109557573A
Authority
CN
China
Prior art keywords
signal
formula
ray
box filter
filter device
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
CN201811448004.0A
Other languages
Chinese (zh)
Other versions
CN109557573B (en
Inventor
胡锐
肖明
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.)
23 Units Of Chinese People's Liberation Army 96901 Force
Original Assignee
China Guangdong Long Source (chengdu) Technology Co Ltd
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 China Guangdong Long Source (chengdu) Technology Co Ltd filed Critical China Guangdong Long Source (chengdu) Technology Co Ltd
Priority to CN201811448004.0A priority Critical patent/CN109557573B/en
Publication of CN109557573A publication Critical patent/CN109557573A/en
Application granted granted Critical
Publication of CN109557573B publication Critical patent/CN109557573B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/20Measuring radiation intensity with scintillation detectors
    • G01T1/203Measuring radiation intensity with scintillation detectors the detector being made of plastics
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01TMEASUREMENT OF NUCLEAR OR X-RADIATION
    • G01T1/00Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
    • G01T1/16Measuring radiation intensity
    • G01T1/20Measuring radiation intensity with scintillation detectors
    • G01T1/204Measuring radiation intensity with scintillation detectors the detector being a liquid

Abstract

A kind of digitlization α/β ray discriminating method, after α/β ray is detected by detector, photomultiplier tube exports current pulse signal, after the conversion of RC feedback-type charge amplifier, two fingers number voltage signal is formed, then carries out digitizing to form digital pulse signal and enter FPGA being handled by ADC;The long Damped exponential signals that RC feedback-type charge amplifier is formed are eliminated using current waveform restorer;Using the parallel digitlization box filter device of building two-way, filter width is arranged according to the die-away time of ZnS (Ag), plastic scintillant, the output signal of current waveform restorer is handled;Peak-holding circuit is for box filter device automatic tracing and exports its peak value;The ratio of two-way peak-holding circuit is obtained using ratio comparator, alpha counter more than given threshold is counted, β counter lower than threshold value is counted, after α/β ray is screened, the counting of output α, β counter increases enable signal certainly, it is waiting to receive from after increasing enable signal, complete counting load.

Description

A kind of digitlization α/β ray discriminating method
Technical field
The invention belongs to radionetric survey technical fields, and in particular to carry out Zhen method for distinguishing for α/β ray to one kind.
Background technique
α/β surface contamination analyzer, Low background α/β measuring instrument can be compound using being made of ZnS (Ag) and plastic scintillant Scintillator and photomultiplier tube, which are constituted, pops one's head in, and α/β ray is carried out while being detected.ZnS (Ag) to Alpha-ray detection efficient very Height, but it is insensitive to β ray, and β radiolucent ZnS (Ag) coating reaches plastic scintillant and is absorbed.Compound scintillator is released Photon current pulse signal is converted to by photomultiplier tube, current signal can be handled by rear class signal processing chain, current impulse The existing alpha signal of signal sequence also has signal beta, and rear class signal processing chain has to screen two kinds of pulse signals in real time, Step-by-step counting can be carried out respectively, achieve the purpose that while measuring α/β ray.
α/β ray is at present there are two types of main discriminating methods: the first is amplitude method, and principle is Alpha-ray signal amplitude Bigger, Beta-ray signal amplitude is smaller, and the threshold value by the way that amplitude comparator is arranged screens two kinds of rays.Second Kind is pulse width method, and principle is the voltage pulse signal that the current signal of photomultiplier tube output is formed after I-V is converted, Alpha-ray pulse width is wider, and Beta-ray pulse width is narrow, by the measurement of pulse-width, can believe two kinds It number is screened.For amplitude method, since α, signal beta have bigger overlapping in amplitude, for overlapping region ray just The case where will appear mutual crosstalk, and since judgment criteria is amplitude, the gain stability of whole system is to particle It is larger to screen influential effect.For pulse width method, the beginning and end location determination of impulse amplitude and baseline noise to pulse Influence it is bigger, cause pulse width measurement inaccuracy, will affect the examination effect of particle.For above two method, also Have a common defect, key is screened parameter and is all controlled by analog device, in amplitude method, the amplitude of pulse by photomultiplier tube, Amplifying circuit is affected, stability influence of the threshold value by reference voltage;In pulse width method, pulse width is by photoelectricity times Increase the influence of the peripheral cell of pipe.Work as environmental change, when device aging, these key parameters can all send out variation, entire to screen effect The stability of fruit is affected.
Summary of the invention
The purpose of the present invention is to provide a kind of digitized α/β ray discriminating method, which can be substantially reduced The influence of signal amplitude, analog device performance change to effect is screened.
In order to solve the above-mentioned technical problem, the present invention is accomplished by the following way:
A kind of digitlization α/β ray discriminating method, specific steps are as follows:
1) after the detector detection that α/β ray is made of scintillator and photomultiplier tube, photomultiplier tube output index The current pulse signal of attenuation function waveform;
2) current pulse signal in step 1) forms double exponential voltages after the conversion of RC feedback-type charge amplifier Signal, while reducing input current pulse signal bandwidth;
3) two fingers number voltage signal is digitized by ADC, and formation digital pulse signal enters FPGA and digitized Signal processing;
4) FPGA described in includes current waveform restorer, box filter device, peak-holding circuit and ratio comparator, first Utilize current waveform restorer removal process 2) long Damped exponential signals that RC feedback-type charge amplifier is formed, allow signal Original current pulse shape is restored to convenient for rear class processing;Then the digitlization box filter device parallel using building two-way, Two filter widths of 2us and 0.2us are set according to the die-away time of ZnS (Ag), plastic scintillant, to current waveform restorer Output signal handled;Peak-holding circuit for box filter device automatic tracing and exports its peak value again;Finally utilize than It is worth the ratio that comparator obtains two-way peak-holding circuit, α/β ray pulse examination is carried out according to ratio, more than the α of given threshold Counter is counted, and the β counter lower than threshold value is counted, and carries out α/β ray pulse examination according to ratio;
5) after α/β ray is screened, the counting of output α, β counter increases enable signal from enable signal, waiting receive is increased certainly Afterwards, counter carries out plus one operates, and completes a counting load.
Compared with prior art, the invention has the benefit that
The parameter that α, β of the invention are screened is only related with the width of the damping time constant of scintillator and Square-Wave Filter, The damping time constant of scintillator is relatively more fixed, and box filter device realizes that parameter is fixed by digital technology.Therefore the screening techniques The influence of parameter during the influence and simulation of signal amplitude can be substantially reduced, and system gain is changed it is insensitive, convenient for adopting It is realized with digital technology, is conducive to the stability of raising system and convenient for debugging production.
Detailed description of the invention
Fig. 1 is digitlization α/β ray discriminating method processing circuit structure chart
Specific embodiment
Specific embodiments of the present invention will be described in further detail in the following with reference to the drawings and specific embodiments.
As shown in Figure 1, α/β ray discriminating method detailed process of the invention:
1) after the detector detection that α/β ray is made of scintillator and photomultiplier tube, photomultiplier tube output index The current pulse signal I of attenuation function waveform(t), express as shown in formula (1);
τ0Scintillator decay time constant, the time attenuation constant of ZnS (Ag) scintillator are 200ns or so, Plastic scintillation Body is tens ns;I0For current impulse maximum value.
2) current pulse signal in step 1) forms double exponential voltages after the conversion of RC feedback-type charge amplifier Signal, while reducing input current pulse signal bandwidth;Convenient for late-class circuit processing, output voltage signal V(t), such as formula (2) institute Show.
A is signal amplitude, τRCIt is RC feedback network curring time, and meets τRC>>τ0
3) two fingers number voltage signal is digitized by ADC (digital analog converter, similarly hereinafter), formed digital pulse signal into Enter FPGA and carry out digitized signal processing, ADC uses the sampling rate of 80M.
4) FPGA includes current waveform restorer, box filter device, peak-holding circuit and ratio comparator, is existed first Using Verilog language building digitlization current waveform restorer removal process 2 in FPGA) RC feedback-type charge amplifier The long Damped exponential signals formed allow signal to be restored to original current pulse shape convenient for rear class processing;Wherein contain sudden strain of a muscle The damping time constant inherent feature of bright body:
Output signal is the frequency-domain expression of formula (2):
Target output signal Q(t)With detector output current wave referring to formula (1), time-domain expression:
The frequency-domain expression of formula (4) are as follows:
Formula (2) signal is by transmission letter h(t)Conversion output type (4) signal, then formula (4) signal be exactly formula (2) with The transfer function h of current waveform restorer(t)Convolution:
Q(t)=V(t)*h(t) (6)
The frequency-domain expression of formula (6) are as follows:
Q(jω)=V(jω)·H(jω) (7)
Bringing formula (3) and formula (5) into formula (7) can export:
Comprising all invariants in formula (8) in COEFFICIENT K, COEFFICIENT K is normalized in the coefficient A ' of output signal, transmits letter Several frequency domain equations:
H(jω)=1+j ω τRC (9)
The continued time domain expression formula of transfer function:
Using the digitlization box filter device that Verilog language building two-way is parallel in FPGA, according to ZnS (Ag), modeling Expect that two filter widths of 2us and 0.2us are arranged in the die-away time of scintillator, two-way box filter device is extensive to current waveform simultaneously The output signal of multiple device is handled;Peak-holding circuit is constructed using Verilog language in FPGA again, for box filter device Automatic tracing simultaneously exports its peak value;The ratio that two-way peak-holding circuit is finally obtained using ratio comparator, is carried out according to ratio α/β ray pulse is screened, and the alpha counter more than given threshold is counted, and the β counter lower than threshold value is counted, according to Ratio carries out α/β ray pulse examination;
The signal exported through current waveform restorer is handled with box filter device, box filter device b(t)Expression formula (11)
T is box filter device width.
Formula (4) signal passes through the receptance function obtained after box filter device are as follows: p (t)
By (13) formula it is found that T > > τ0When p (t) reach maximum value A ' τ 0, otherwise amplitude peak is
Using two-way box filter device parallel processing, the width of two box filter devices is different, if wider rectangular Filter uses width T1>>τ0, relatively narrow box filter device width T2With τ0Quite, two filters can be derived according to above-mentioned conclusion The ratio R of wave device output signal are as follows:
By formula (14) it is found that the ratio of the output signal of two box filter devices, only with the width of relatively narrow Square-Wave Filter It is related with the damping time constant of scintillator, it is unrelated with signal amplitude.
Wider box filter device width T1For 2us, relatively narrow box filter device width T2For 0.2us, β ray is by plastics Scintillator detection, the current impulse time constant of formation are only tens ns, and the signal amplitude ratio of two box filter devices output connects It is bordering on 1.Alpha ray is detected by ZnS (Ag) scintillator, and the current impulse time constant of formation is 0.2us, and two Square-Wave Filters are defeated Signal, using amplitude ratio, can screen two kinds of particles than about 1.5 times out.
5) after α/β ray is screened, the counting of output α, β counter increases enable signal from enable signal, waiting receive is increased certainly Afterwards, counter carries out plus one operates, and completes a counting load.
The above is only embodiments of the present invention, is stated again, and those skilled in the art are come It says, without departing from the principle of the present invention, several improvement can also be carried out to the present invention, these improvement are also included in the present invention In scope of protection of the claims.

Claims (3)

1. a kind of digitlization α/β ray discriminating method, it is characterised in that: itself specific steps are as follows:
1) after the detector detection that α/β ray is made of scintillator and photomultiplier tube, the decaying of photomultiplier tube output index The current pulse signal I of function waveform(t)As shown in formula (1):
τ0Scintillator decay time constant, I0For current impulse maximum value;
2) current pulse signal in step 1) forms double exponential voltage letters after the conversion of RC feedback-type charge amplifier Number, while input current pulse signal bandwidth is reduced, it is handled convenient for late-class circuit, output voltage signal V(t)As shown in formula (2):
A is signal amplitude, τRCIt is RC feedback network curring time, and meets τRC>>τ0
3) two fingers number voltage signal is digitized by ADC, is formed digital pulse signal and is entered FPGA progress digitized signal Processing;
4) FPGA described in includes current waveform restorer, box filter device, peak-holding circuit and ratio comparator, first with Current waveform restorer removal process 2) RC feedback-type charge amplifier formed long Damped exponential signals, allow signal to restore To original current pulse shape convenient for rear class processing;Then the digitlization box filter device parallel using building two-way, according to Die-away time setting two filter widths of 2us and 0.2us of ZnS (Ag), plastic scintillant, to the defeated of current waveform restorer Signal is handled out;Peak-holding circuit for box filter device automatic tracing and exports its peak value again;Finally utilize odds ratio Compared with the ratio that device obtains two-way peak-holding circuit, α/β ray pulse examination is carried out according to ratio, the α more than given threshold is counted Device is counted, and the β counter lower than threshold value is counted, and carries out α/β ray pulse examination according to ratio;
5) after α/β ray is screened, the counting of output α, β counter increases enable signal certainly, waiting to receive from after increasing enable signal, meter Number device carries out plus an operation, completes a counting load.
2. a kind of digitlization α/β ray discriminating method according to claim 1, it is characterised in that: packet in the step 4) Contained the damping time constant inherent feature of scintillator: output signal is the frequency-domain expression of formula (2):
Target output signal Q(t)With detector output current wave referring to formula (1), time-domain expression:
The frequency-domain expression of formula (4) are as follows:
Formula (2) signal is by transmission letter h(t)Conversion output type (4) signal, then formula (4) signal is exactly formula (2) and electric current The transfer function h of waveform restorer(t)Convolution:
Q(t)=V(t)*h(t) (6)
The frequency-domain expression of formula (6) are as follows:
Q(jω)=V(jω)·H(jω) (7)
Bringing formula (3) and formula (5) into formula (7) can export:
Comprising all invariants in formula (8) in COEFFICIENT K, COEFFICIENT K is normalized in the coefficient A ' of output signal, transfer function Frequency domain equation:
H(jω)=1+j ω τRC (9)
The continued time domain expression formula of transfer function:
3. a kind of digitlization α/β ray discriminating method according to claim 2, it is characterised in that: through electricity in the step 4 The signal of stream waveform restorer output is handled with box filter device, the expression formula (11) of box filter device b (t)
Formula (4) signal passes through the receptance function obtained after box filter device are as follows: p (t)
Using two-way box filter device parallel processing, the width of two box filter devices is different, and wider box filter device is adopted With width T1>>τ0, relatively narrow box filter device width T2With τ0Quite, two filter outputs can be derived according to above-mentioned conclusion The ratio R of signal are as follows:
By formula (14) it is found that the ratio of the output signal of two box filter devices, only with the width of relatively narrow Square-Wave Filter and sudden strain of a muscle The damping time constant of bright body is related, and β ray is detected by plastic scintillant, and the signal amplitude ratio of two box filter devices output connects It is bordering on 1, alpha ray is detected by ZnS (Ag) scintillator, and the current impulse time constant of formation is 0.2us, and two Square-Wave Filters are defeated Signal, using amplitude ratio, can screen two kinds of particles than about 1.5 times out.
CN201811448004.0A 2018-11-29 2018-11-29 Digital alpha/beta ray discrimination method Active CN109557573B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201811448004.0A CN109557573B (en) 2018-11-29 2018-11-29 Digital alpha/beta ray discrimination method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201811448004.0A CN109557573B (en) 2018-11-29 2018-11-29 Digital alpha/beta ray discrimination method

Publications (2)

Publication Number Publication Date
CN109557573A true CN109557573A (en) 2019-04-02
CN109557573B CN109557573B (en) 2022-07-15

Family

ID=65868118

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201811448004.0A Active CN109557573B (en) 2018-11-29 2018-11-29 Digital alpha/beta ray discrimination method

Country Status (1)

Country Link
CN (1) CN109557573B (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110068855A (en) * 2019-05-23 2019-07-30 上海仁机仪器仪表有限公司 Multi-functional ray detector and its assemble method based on MPPC
CN111025373A (en) * 2019-12-26 2020-04-17 中广核久源(成都)科技有限公司 Method for digitally correcting decay time of sodium iodide crystal in real time
CN111060982A (en) * 2019-12-27 2020-04-24 中广核久源(成都)科技有限公司 Front radiation detector for X-ray machine
CN111404542A (en) * 2020-03-31 2020-07-10 四川新先达测控技术有限公司 Double-exponential nuclear signal counting method and device
CN112327347A (en) * 2020-10-29 2021-02-05 中广核久源(成都)科技有限公司 Digital nuclear pulse forming system with adjustable curvature
CN112946721A (en) * 2021-01-22 2021-06-11 西安交通大学 Detector capable of simultaneously identifying alpha, beta and gamma rays and detection method

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57119275A (en) * 1981-01-19 1982-07-24 Aloka Co Ltd Discriminating circuit for radiation detecting wave form
US4454587A (en) * 1981-04-25 1984-06-12 Kernforschungszentrum Karlsruhe Gesellschaft Mit Beschrankter Haftung Method and circuit arrangement for discriminating between pulses generated by alpha and/or beta radiators
JPS62287177A (en) * 1986-06-06 1987-12-14 Nippon Atom Ind Group Co Ltd Monitor for iodine 129
JP2002116135A (en) * 2000-10-10 2002-04-19 Fuji Electric Co Ltd Electronic circuit for fine particle counting turbidimeter and for fine particle counter
CN101063664A (en) * 2006-04-27 2007-10-31 北京市射线应用研究中心 Method and device for monitoring radioactivity artificial aerosol
CN105319574A (en) * 2015-11-16 2016-02-10 中国原子能科学研究院 An alpha and beta pulse discriminating method
CN206020674U (en) * 2016-08-30 2017-03-15 中广核久源(成都)科技有限公司 A kind of portable Low background α, β measuring instrument
CN207408601U (en) * 2017-11-02 2018-05-25 中广核久源(成都)科技有限公司 A kind of neutron based on CLYC crystal, gamma dose measurement system

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57119275A (en) * 1981-01-19 1982-07-24 Aloka Co Ltd Discriminating circuit for radiation detecting wave form
US4454587A (en) * 1981-04-25 1984-06-12 Kernforschungszentrum Karlsruhe Gesellschaft Mit Beschrankter Haftung Method and circuit arrangement for discriminating between pulses generated by alpha and/or beta radiators
JPS62287177A (en) * 1986-06-06 1987-12-14 Nippon Atom Ind Group Co Ltd Monitor for iodine 129
JP2002116135A (en) * 2000-10-10 2002-04-19 Fuji Electric Co Ltd Electronic circuit for fine particle counting turbidimeter and for fine particle counter
CN101063664A (en) * 2006-04-27 2007-10-31 北京市射线应用研究中心 Method and device for monitoring radioactivity artificial aerosol
CN105319574A (en) * 2015-11-16 2016-02-10 中国原子能科学研究院 An alpha and beta pulse discriminating method
CN206020674U (en) * 2016-08-30 2017-03-15 中广核久源(成都)科技有限公司 A kind of portable Low background α, β measuring instrument
CN207408601U (en) * 2017-11-02 2018-05-25 中广核久源(成都)科技有限公司 A kind of neutron based on CLYC crystal, gamma dose measurement system

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
唐恭富 等: "基于大面积复合闪烁体的α、β射线甄别电路设计", 《兵器装备工程学报》 *

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110068855A (en) * 2019-05-23 2019-07-30 上海仁机仪器仪表有限公司 Multi-functional ray detector and its assemble method based on MPPC
CN111025373A (en) * 2019-12-26 2020-04-17 中广核久源(成都)科技有限公司 Method for digitally correcting decay time of sodium iodide crystal in real time
CN111025373B (en) * 2019-12-26 2023-03-31 中广核久源(成都)科技有限公司 Method for digitally correcting decay time of sodium iodide crystal in real time
CN111060982A (en) * 2019-12-27 2020-04-24 中广核久源(成都)科技有限公司 Front radiation detector for X-ray machine
CN111404542A (en) * 2020-03-31 2020-07-10 四川新先达测控技术有限公司 Double-exponential nuclear signal counting method and device
CN112327347A (en) * 2020-10-29 2021-02-05 中广核久源(成都)科技有限公司 Digital nuclear pulse forming system with adjustable curvature
CN112946721A (en) * 2021-01-22 2021-06-11 西安交通大学 Detector capable of simultaneously identifying alpha, beta and gamma rays and detection method

Also Published As

Publication number Publication date
CN109557573B (en) 2022-07-15

Similar Documents

Publication Publication Date Title
CN109557573A (en) A kind of digitlization α/β ray discriminating method
CN103969675B (en) Digitize the baseline correction method and system of scintillation pulse
US5067090A (en) Nuclear spectroscopy method and apparatus for digital pulse height analysis
CN103336293B (en) A kind of method optimizing liquid scintillation bulk detector examination neutron and gamma ability
CN106547017A (en) A kind of compound scintillator gamma ray spectrometer
CN111025373B (en) Method for digitally correcting decay time of sodium iodide crystal in real time
US5349195A (en) Spectroscopy method for high count rate nuclear pulses
CN111553111B (en) Digital imitation nuclear signal generator based on MCNP
Esmaeili-Sani et al. Triangle bipolar pulse shaping and pileup correction based on DSP
Xiaohui et al. Analysis of three digital n/γ discrimination algorithms for liquid scintillation neutron spectrometry
CN205176285U (en) Anticoincidence output system of examineing
CN106772540A (en) A kind of hard X ray flux detecting system of J TEXT tokamak devices
CN108008438B (en) Ray energy measuring device and method
CN115420226A (en) Ray action position positioning device and method based on pulse width
CN105492929B (en) Radiation detecting apparatus and radiation dose measurement processing method
CN111239797B (en) Collector based on radiation particle event and rapid nuclide identification method
CN111505696A (en) Double-time-step pileup waveform processing system and method
CN116466384B (en) Method and device for processing scintillation pulse, electronic equipment and storage medium
Paul et al. Implementation of FPGA based real-time digital DAQ for high resolution, and high count rate nuclear spectroscopy application
DE3635477A1 (en) METHOD AND CIRCUIT ARRANGEMENT FOR REDUCING THE NUMBER OF SUBSTANCES OF THE MEASUREMENT WITH A CONCENTENCE-ANTICO-INCIDENCE EVALUATION
Szadkowski et al. DAQ Golden Rules in the Anti-Aliasing Bessel Filter vs. Potentially Lost Events in the Surface Detectors in Cosmic Rays Experiments
CN114254495B (en) Monte Carlo method-based simulated energy spectrum generation method
Vaghela et al. FPGA Implementation of Digital pulse processing techniques for Radiation Measurement
He et al. A ratio pulse-shape discriminator
Singh DSP Techniques for Neutron-Gamma Discrimination by Liquid Organic Scintillators

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
CB03 Change of inventor or designer information

Inventor after: Hu Rui

Inventor after: Xiao Ming

Inventor after: Yang Binhua

Inventor after: Zhao Fengtao

Inventor after: Deng Yunyue

Inventor after: Zhang Kai

Inventor before: Hu Rui

Inventor before: Xiao Ming

CB03 Change of inventor or designer information
TA01 Transfer of patent application right

Effective date of registration: 20220421

Address after: 610000 Building 2, No. 21, Gaopeng Avenue, Chengdu, Sichuan

Applicant after: CGN JIUYUAN (CHENGDU) TECHNOLOGY CO.,LTD.

Applicant after: 23 Units of the Chinese People's Liberation Army 96901 Force

Address before: 610000 Industrial Concentration Zone of Southwest Airport Economic Development Zone, Shuangliu District, Chengdu City, Sichuan Province

Applicant before: CGN JIUYUAN (CHENGDU) TECHNOLOGY CO.,LTD.

TA01 Transfer of patent application right
GR01 Patent grant
GR01 Patent grant