CN202216921U - Digital positron annihilation life spectrometer device - Google Patents

Digital positron annihilation life spectrometer device Download PDF

Info

Publication number
CN202216921U
CN202216921U CN2011202928863U CN201120292886U CN202216921U CN 202216921 U CN202216921 U CN 202216921U CN 2011202928863 U CN2011202928863 U CN 2011202928863U CN 201120292886 U CN201120292886 U CN 201120292886U CN 202216921 U CN202216921 U CN 202216921U
Authority
CN
China
Prior art keywords
conversion circuit
photomultiplier
speed
positron annihilation
high voltage
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.)
Expired - Fee Related
Application number
CN2011202928863U
Other languages
Chinese (zh)
Inventor
成斌
叶邦角
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.)
University of Science and Technology of China USTC
Original Assignee
University of Science and Technology of China USTC
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 University of Science and Technology of China USTC filed Critical University of Science and Technology of China USTC
Priority to CN2011202928863U priority Critical patent/CN202216921U/en
Application granted granted Critical
Publication of CN202216921U publication Critical patent/CN202216921U/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Landscapes

  • Measurement Of Radiation (AREA)

Abstract

The utility model relates to a digital positron annihilation life spectrometer device which is composed of a first photomultiplier tube (1), a second photomultiplier tube (11), a first high voltage power supplier (2), a second high voltage power supplier (12), a first flashing body (3), a second flashing body (13), a clamping source for material to be tested (4), a high-speed analog-to-digital conversion circuit main board (5), a high-speed analog-to-digital conversion circuit secondary board (6), a bridge circuit (7) and a computer (8). According to the digital positron annihilation life spectrometer device, the structure of the positron annihilation life spectrometer is greatly simplified, the reliability of the instruments is improved, and the construction cost is reduced; and meanwhile, the spectrometer has the advantages of low noise, long-time stable performance, small environment temperature influence, flexible online or offline data processing, automatic search of an optimal energy window, and the like.

Description

A kind of digitizing positron annihilation life spectrometer device
Technical field
The utility model belongs to the applied nuclear technologies field, is specifically related to a kind of digitizing positron annihilation life spectrometer device.
Background technology
Conventional positron life spectrometer is by scintillator probe, high voltage supply device, constant proportion timing discrminator, fast coincidence circuit, time-delay case, time-amplitude analyzer, NIM cabinet, microcomputer multichannel card; Computing machine is formed; Wherein constant proportion timing discrminator, fast coincidence circuit, time-amplitude analyzer belong to the plug-in unit of NIM cabinet, and the microcomputer multichannel card is inserted in the PCI slot of computing machine.The scintillator probe detection is behind gamma-rays; Get into CFD from negative signal of probe anode output; Accomplish two parts work by CFD; A part of work is carried out amplitude discriminator to input signal, when input signal amplitude meets up and down threshold range, export one by the definite standard SCA signal of constant proportion timing method.Next in CFD, be divided into two-way SCA output signal: one tunnel output positive signal is used for meeting soon to trigger enabling signal, and another road output negative signal gets into TAC after time delay.When meeting the out gate signal soon to behind the TAC; The TAC of two-way SCA signal will convert the signal that is directly proportional with amplitude the mistiming to; Range signal is converted into numerical value is stored at last in the computer storage hardware thereby carry out amplitude discriminator by MCA, it is the positron life spectrum that some such incidents are accumulated resulting composing.
Conventional positron annihilation life spectrometer needs more NIM plug-in unit; Setting up debugging needs long time, as long as one of them plug-in unit goes wrong, a whole set of spectrometer cannot normally use; The maintenance of spectrometer need be especially careful, and the expense of setting up a cover spectrometer simultaneously is also higher.When spectrometer was worked, the NIM plug-in unit was acted upon by temperature changes bigger, need be operated under the constant temperature.Because Data Acquisition belongs to online treatment, system's dead time of this kind mode is less, but when a part of data in the measurement go wrong, must from the beginning remeasure, and its processing method of data is also confirmed by hardware is unique.
The utility model content
The purpose of the utility model is for the establishment that makes spectrometer simply saves time, and the reduction construction cost is easy to maintenance, reduces to receive the influence of environment temperature, has data processing method more flexibly.
The technical solution that the utility model is taked is following:
A kind of digitizing positron annihilation life spectrometer device is made up of first photomultiplier 1, second photomultiplier 11, the first high voltage supply device 2, the second high voltage supply device 12, primary scintillator 3, secondary fluor 13, test substance folder source 4, high-speed A/D conversion circuit mainboard 5, high-speed A/D conversion circuit slave plate 6, bridgt circuit 7, computing machine 8;
The first high voltage supply device 2, the second high voltage supply device 12 connect with first photomultiplier, 1, the second photomultiplier 11 respectively;
Primary scintillator 3, secondary fluor 13 through transmissivity greater than 95%, refractive index greater than 1.3 optics silicone oil respectively with first photomultiplier 1,11 couplings of second photomultiplier, with the aluminum hull encapsulation, guarantee the light leakproofness again;
The output signal of first photomultiplier 1 is connected to the input end of analog signal of high-speed A/D conversion circuit mainboard 5 through concentric cable;
The output signal of second photomultiplier 11 is connected to the input end of analog signal of high-speed A/D conversion circuit slave plate 6 through concentric cable;
High-speed A/D conversion circuit mainboard 5 is connected through bridgt circuit 7 with high-speed A/D conversion circuit slave plate 6;
High-speed A/D conversion circuit mainboard 5 is connected with computing machine 8 through pci bus interface with high-speed A/D conversion circuit slave plate 6.
The good effect of the utility model is:
The positron annihilation life spectrometer of the routine that compares; We have simplified the spectrometer structure by the digitizing positron annihilation life spectrometer of development greatly; Do not re-use corresponding N IM plug-in unit; Replace with the high-speed figure capture card, setting up of spectrometer become with debugging simply save time, greatly strengthened the reliability of instrument.Reduced the construction cost of spectrometer, spectrometer is promoted in application market more easily.Simultaneously, this cover digitizing positron annihilation life spectrometer also has low noise, and long-time stable performance receives the temperature effect of environment less, and online flexibly or off-line data is handled, and can obtain more physical message as required.Can realize the storage of raw data very easily, carry out off-line data and handle, improve the service efficiency of spectrometer.Utilize digitized characteristics, the method that no longer needs manually to survey power spectrum is regulated Canon window.And make into as required, seek optimized ability window automatically through the life spectrum of measurement standard sample after the appointment relevant parameter, further improve the performance and the efficient of instrument.
Description of drawings
Fig. 1 is the utility model structural drawing.
Embodiment
Below in conjunction with Figure of description the utility model is further specified.
At first use the identical object under test of two thickness with the positron emission source 22Na is clipped in the middle, and object under test thickness generally requires greater than 1mm, 22Na source radioactivity is greatly about tens microcurie magnitudes.The gamma-ray photon detector that is made up of photomultiplier 1,11 and BaF2 scintillator 3,13 is placed in test substance folder 4 both sides, source, survey respectively by 22The Na radioactive source sends gamma-ray photon that energy that positron decay produces is 1.28MeV and positron, and in object under test, to fall into oblivion the energy that produces be the gamma-ray photon of 511keV, i.e. the start signal of positron annihilation and termination signal.Wherein, BaF2 scintillator volume is φ 30 * 15mm, and greater than 95%, refractive index is coupled greater than 1.3 optics silicone oil and photomultiplier, guarantees the light leakproofness with the aluminum hull encapsulation again through transmissivity.When the BaF2 scintillator receives gamma-ray photon, can change into the receivable fluorescent photon of photomultiplier to gamma-ray photon, the time level of photomultiplier at first is converted into a spot of electronics with it after receiving fluorescent photon.The high voltage supply device 2,12 that is connected with photomultiplier 1,11 can be taken between the level each dozen of photomultiplier and form electric field; Under this effect of electric field; Time,, the little electrons sent of level was accelerated multiplication; Final produce an amplitude, by the anode of photomultiplier or beat and take level to export the energy positive correlation of its amplitude and gamma-ray photon greatly about the electric impulse signal of several V.Wherein, the high pressure of high voltage supply device 2,12 is greatly about several kilovolts, and rated current is at several mA.
The electric signal that is produced by photomultiplier transmits through concentric cable, can effectively avoid the space electromagnetic interference (EMI).The signal of two photomultipliers is transferred to high-speed A/D conversion circuit ADC mainboard 5 and high-speed A/D conversion circuit slave plate 6 respectively, by analog to digital conversion circuit simulating signal is carried out high-speed sampling, is converted into digital signal and is stored in plate and carry in the buffer memory.High-speed ADC mainboard 5 is connected through bridgt circuit 7 with high-speed ADC slave plate 6, guarantees the clock synchronization of high-speed ADC mainboard 5 and high-speed ADC slave plate 6, reduces the time measurement error.High-speed ADC satisfies sampling rate greater than 2GS/s here, and bandwidth is greater than 1GHz.High-speed ADC mainboard 5 all passes through pci interface with high-speed ADC slave plate 6 and links to each other with computing machine.Write when full when plate carries buffer memory, by programmed control plate is carried and data cachedly write calculator memory or hard disk, and empty plate and carry buffer memory and work on.
After obtaining digital signal, can select online signal Processing as required perhaps with carrying out processed offline behind the data-storing.No matter online treatment or processed offline all are to use self-compiling program that the signal waveform that obtains is handled automatically.At first screen and declare choosing, promptly to being start signal, termination signal or noise according to judgement received signals such as amplitude areas behind the waveform fitting.The selected appropriate threshold of Automatic Program will be declared the real event example signal of selecting and carry out digital constant proportion regularly after judging.Soon the certain proportion value of the amplitude of match afterpulse waveform is as standard, and like 20% of range value, pulse front edge promptly is decided to be the zero-time of this pulse in the position at this standard value place.This kind timing method can effectively reduce the amplitude autokinetic effect to time-resolved influence.
When a large amount of examples of accumulation, the mistiming of calculating start signal and termination signal, make after the statistical Butut, just can obtain the annihilation life spectrum of positron in test substance.

Claims (1)

1. digitizing positron annihilation life spectrometer device is characterized in that: affiliated digitizing positron annihilation life spectrometer device is made up of first photomultiplier (1), second photomultiplier (11), the first high voltage supply device (2), the second high voltage supply device (12), primary scintillator (3), secondary fluor (13), test substance folder source (4), high-speed A/D conversion circuit mainboard (5), high-speed A/D conversion circuit slave plate (6), bridgt circuit (7), computing machine (8);
The first high voltage supply device (2), the second high voltage supply device (12) are connected with first photomultiplier (1), second photomultiplier (11) respectively;
Primary scintillator (3), secondary fluor (13) through transmissivity greater than 95%, refractive index greater than 1.3 optics silicone oil respectively with first photomultiplier (1), second photomultiplier (11) coupling, with the aluminum hull encapsulation, guarantee the light leakproofness again;
The output signal of first photomultiplier (1) is connected to the input end of analog signal of high-speed A/D conversion circuit mainboard (5) through concentric cable;
The output signal of second photomultiplier (11) is connected to the input end of analog signal of high-speed A/D conversion circuit slave plate (6) through concentric cable;
High-speed A/D conversion circuit mainboard (5) is connected through bridgt circuit (7) with high-speed A/D conversion circuit slave plate (6);
High-speed A/D conversion circuit mainboard (5) is connected with computing machine (8) through pci bus interface with high-speed A/D conversion circuit slave plate (6).
CN2011202928863U 2011-08-12 2011-08-12 Digital positron annihilation life spectrometer device Expired - Fee Related CN202216921U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN2011202928863U CN202216921U (en) 2011-08-12 2011-08-12 Digital positron annihilation life spectrometer device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN2011202928863U CN202216921U (en) 2011-08-12 2011-08-12 Digital positron annihilation life spectrometer device

Publications (1)

Publication Number Publication Date
CN202216921U true CN202216921U (en) 2012-05-09

Family

ID=46016169

Family Applications (1)

Application Number Title Priority Date Filing Date
CN2011202928863U Expired - Fee Related CN202216921U (en) 2011-08-12 2011-08-12 Digital positron annihilation life spectrometer device

Country Status (1)

Country Link
CN (1) CN202216921U (en)

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102680500A (en) * 2012-05-30 2012-09-19 武汉大学 Positron average lifetime decomposing method
CN103033523A (en) * 2012-12-17 2013-04-10 中国科学院高能物理研究所 Novel positron annihilation spectrometer and measurement method thereof
CN106680300A (en) * 2017-01-17 2017-05-17 武汉大学 Multidimensional positron annihilation lifetime spectrum and doppler broadening spectrum measurement systems
CN109997030A (en) * 2016-11-16 2019-07-09 恩德莱斯和豪瑟尔欧洲两合公司 Method for determining the remaining run the period of detector cell
CN110988628A (en) * 2019-12-09 2020-04-10 西北核技术研究院 Method for detecting insulating property of dielectric material by positron annihilation technology
CN111024743A (en) * 2019-12-19 2020-04-17 南昌大学 Device and method for waveform sampling of positron life spectrum
CN113640852A (en) * 2021-09-18 2021-11-12 中国科学技术大学 Positron annihilation life spectrometer for measuring film sample
CN113655513A (en) * 2021-08-16 2021-11-16 中国科学技术大学 Digitized anti-coincidence multi-path interaction-starting positron annihilation life spectrometer

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102680500A (en) * 2012-05-30 2012-09-19 武汉大学 Positron average lifetime decomposing method
CN102680500B (en) * 2012-05-30 2014-05-21 武汉大学 Positron average lifetime decomposing method
CN103033523A (en) * 2012-12-17 2013-04-10 中国科学院高能物理研究所 Novel positron annihilation spectrometer and measurement method thereof
CN109997030A (en) * 2016-11-16 2019-07-09 恩德莱斯和豪瑟尔欧洲两合公司 Method for determining the remaining run the period of detector cell
CN109997030B (en) * 2016-11-16 2022-01-28 恩德莱斯和豪瑟尔欧洲两合公司 Method for determining a remaining operating period of a detector unit
CN106680300A (en) * 2017-01-17 2017-05-17 武汉大学 Multidimensional positron annihilation lifetime spectrum and doppler broadening spectrum measurement systems
CN106680300B (en) * 2017-01-17 2019-04-09 武汉大学 Various dimensions positron annihilation lifetime spectrum and dopplerbroadening spectral measurement system
CN110988628A (en) * 2019-12-09 2020-04-10 西北核技术研究院 Method for detecting insulating property of dielectric material by positron annihilation technology
CN111024743A (en) * 2019-12-19 2020-04-17 南昌大学 Device and method for waveform sampling of positron life spectrum
CN113655513A (en) * 2021-08-16 2021-11-16 中国科学技术大学 Digitized anti-coincidence multi-path interaction-starting positron annihilation life spectrometer
CN113640852A (en) * 2021-09-18 2021-11-12 中国科学技术大学 Positron annihilation life spectrometer for measuring film sample

Similar Documents

Publication Publication Date Title
CN202216921U (en) Digital positron annihilation life spectrometer device
US11944470B2 (en) Method and device for sampling a pulse signal, and computer program medium
CN101937096A (en) Multi-channel pulse amplitude analyzer
Akimov et al. The ZEPLIN-III anti-coincidence veto detector
Modamio et al. Digital pulse-timing technique for the neutron detector array NEDA
CN105958955B (en) Signal amplifier and its positron annihilation lifetime measurement system
Cieślak et al. Pulse shape discrimination characteristics of stilbene crystal, pure and 6Li loaded plastic scintillators for a high resolution coded-aperture neutron imager
Cooper et al. Phase i upgrade of the cms hadron calorimeter
Garcia et al. MONSTER: a time of flight spectrometer for β-delayed neutron emission measurements
CN201600461U (en) Multichannel pulse amplitude analyzer
CN109557575A (en) A kind of neutron multiplicity measuring device and its application method
CN103529470B (en) A kind of nuclear radiation detection system and method being applied to field of safety check
CN113109861A (en) Radiation detection device and method thereof
Popov et al. Lithium glass scintillator neutron detector as an improved alternative to the standard 3 he proportional counter
Satoh Development of a New Exclusive Function for a 2012 Model 6Li Time Analyzer Neutron Detector System
CN205176285U (en) Anticoincidence output system of examineing
Canet et al. Digital front-end electronics for the neutron detector NEDA
Wainberg et al. Digital electronics for the Pierre Auger Observatory AMIGA muon counters
Franke Searching for reactor antineutrino flavor oscillations with the double chooz far detector
Onel et al. CMS Hadron Forward Calorimeter Phase I Upgrade Status
CN103068135B (en) Time of exposure non-intervention measuring device and method of X-ray machine
Lucht Installation, commissioning and performance of the trigger system of the Double Chooz experiment and the analysis of hydrogen capture neutrino events
CN110646830A (en) Digital signal processing system of tokamak anti-compton gamma energy spectrometer
CN101923062A (en) Mobile type digital positron life spectrometer
Ruede New Peak Finding Algorithm for the BCM1F Detector of the CMS Experiment at CERN

Legal Events

Date Code Title Description
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20120509

Termination date: 20200812