CN108196293A - One kind is based on scintillator detector dosage rate detection method - Google Patents
One kind is based on scintillator detector dosage rate detection method Download PDFInfo
- Publication number
- CN108196293A CN108196293A CN201810209495.7A CN201810209495A CN108196293A CN 108196293 A CN108196293 A CN 108196293A CN 201810209495 A CN201810209495 A CN 201810209495A CN 108196293 A CN108196293 A CN 108196293A
- Authority
- CN
- China
- Prior art keywords
- measured
- section
- pulsewidth
- scintillator detector
- sections
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01T—MEASUREMENT OF NUCLEAR OR X-RADIATION
- G01T1/00—Measuring X-radiation, gamma radiation, corpuscular radiation, or cosmic radiation
- G01T1/02—Dosimeters
- G01T1/023—Scintillation dose-rate meters
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- General Physics & Mathematics (AREA)
- High Energy & Nuclear Physics (AREA)
- Molecular Biology (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Measurement Of Radiation (AREA)
Abstract
The present invention discloses a kind of based on scintillator detector dosage rate detection method, this method is in unit measuring section, according to different pulse characteristics, different pulse widths is divided into three sections, count the counting in each pulsewidth section, calculate the reference radiation calibration factor of corresponding pulsewidth so that required radiation dose rate measurement error smaller to be measured, more accurate.
Description
Technical field
The present invention relates to nuclear radiation detection more particularly to applied in X, gamma Rays dosage field of detecting.
Background technology
Due to ray radiant energy difference, the electric impulse signal width t that scintillator detector is converted out is also different, corresponding institute
The reference radiation calibration factor Y asked is also different.In scintillator detector radiation dose rate measuring technique, radiation dose rate to be measured
H*It is related with the step-by-step counting N and reference radiation calibration factor Y that unit interval counts on.And traditional scintillator detector spoke
Penetrate Dose rate measurement method be then in order to reduce survey calculation amount, to different-energy pulsewidth all with same reference radiation calibrate because
Sub- Y empirical values calculate required radiation dose rate H*, eventually lead to radiation dose rate H to be measured*Measurement error is big, inaccurate.
Invention content
In view of the above-mentioned deficiencies in the prior art, the purpose of the present invention is to propose to one kind to be based on scintillator detector agent
Dose rate detection method.The detection method feature is in unit measuring section, according to different pulse characteristics, by different arteries and veins
It rushes width and is divided into three sections, count the counting in each pulsewidth section, calculate the reference radiation calibration factor of corresponding pulsewidth, make
Required radiation dose rate measurement error smaller to be measured, more accurate.
The technical scheme is that:One kind is based on scintillator detector dosage rate detection method, step:1. due to spoke
It is directly proportional to pulse signal width to penetrate energy size, it, can will be after the interaction of scintillator and ray in unit measuring section T
The electric impulse signal converted out is divided into three sections according to different pulse signal widths;
2. being measured in reference instrument respectively three times, count and three pulsewidths are corresponded in each unit measuring section T
The step-by-step counting N in sectiontn, wherein three pulsewidth section t=1,2,3, pendulous frequency n=1,2,3, i.e., measure what is counted three times
It is respectively N that three distinct pulse widths, which count,11、N21、N31, N12、N22、N32, N13、N23、N33;
3. the radiation dose rate measured in the known reference instrument three times is respectively H1、H2、H3, surveyed described three times
Measure the step-by-step counting N corresponding to the three section pulsewidths counted1n、N2n、N3nSubstitution formula Hn=N1n*Y1+N2n*Y2+N3n*Y3In,
Ternary linear function group is formed, the reference radiation calibration factor Y to be measured corresponding to these three pulsewidth sections is obtainedt, wherein three
Pulsewidth section t=1,2,3, ternary linear function group is as follows:
Ternary linear function group is solved,
4. in unit measuring section T, measure corresponding to three pulsewidth sections in statistics scintillator detector instrument
Step-by-step counting N1、N2、N3;
5. by required radiometric calibration factor Y in 3.1、Y2、Y34. in three pulsewidths counted are measured in instrument to be measured
Step-by-step counting N corresponding to section1、N2、N3Substitution formula H*=N1*Y1+N2*Y2+N3*Y3In, you can it is to be measured that scintillator detector is obtained
Dosage rate H*。
In unit measuring section T, the pulse width section measured by scintillator detector is not limited to be divided into three
Section, the actual pulse signal width feature that can also be gone out according to different scintillators and radiation detection intensity-conversion are divided.Its
Middle pulses of radiation width section hop count divides more, then corresponding required reference radiation calibration factor number is more, then
The measured value of scintillator detector radiation dose rate is more accurate.
The advantage of the invention is that:Employ above-mentioned technical solution so that in the detection of scintillator detector dosage rate more
It is accurate.For conventional radiation dosage rate detection method, the dosage rate detection method be in unit measuring section,
According to different pulse characteristics, different pulse widths is divided into three sections, counts the counting in each pulsewidth section, calculating pair
Answer the reference radiation calibration factor of pulsewidth so that required radiation dose rate measurement error smaller to be measured, more accurate.
Description of the drawings
Fig. 1 is the detector radiation dose rate detection method flow chart of the present invention.
Specific embodiment
One kind proposed by the present invention is illustrated such as in conjunction with the accompanying drawings and embodiments based on scintillator detector dosage rate detection method
Under.
With reference to figure 1, mainly comprising the following steps for the method for the present invention is used:
It 1., can be by scintillator in unit measuring section T since radiation energy size is directly proportional to pulse signal width
The electric impulse signal converted out after interacting from ray can be divided into three sections according to different pulse signal widths;
2. being measured in reference instrument respectively three times, count and three pulsewidths are corresponded in each unit measuring section T
The step-by-step counting N in sectiontn, wherein three pulsewidth section t=1,2,3, pendulous frequency n=1,2,3, i.e., measure what is counted three times
It is respectively N that three distinct pulse widths, which count,11、N21、N31, N12、N22、N32, N13、N23、N33;
3. the radiation dose rate measured in the known reference instrument three times is respectively H1、H2、H3, surveyed described three times
Measure the step-by-step counting N corresponding to the three section pulsewidths counted1n、N2n、N3nSubstitution formula Hn=N1n*Y1+N2n*Y2+N3n*Y3In,
Ternary linear function group is formed, the reference radiation calibration factor Y to be measured corresponding to these three pulsewidth sections is obtainedt, wherein three
Pulsewidth section t=1,2,3, ternary linear function group is as follows:
Ternary linear function group is solved,
4. in unit measuring section T, measure corresponding to three pulsewidth sections in statistics scintillator detector instrument
Step-by-step counting N1、N2、N3;
5. by required radiometric calibration factor Y in 3.1、Y2、Y34. in three pulsewidths counted are measured in instrument to be measured
Step-by-step counting N corresponding to section1、N2、N3Substitution formula H*=N1*Y1+N2*Y2+N3*Y3In, you can it is to be measured that scintillator detector is obtained
Dosage rate H*。
Claims (2)
1. one kind is based on scintillator detector dosage rate detection method, step:1. due to radiation energy size and pulse signal
Width is directly proportional, in unit measuring section T, can by the electric impulse signal converted out after scintillator and ray interaction by
Three sections are divided into according to different pulse signal widths;
2. being measured in reference instrument respectively three times, count and three pulsewidth sections are corresponded in each unit measuring section T
Step-by-step counting Ntn, wherein three pulsewidth section t=1,2,3, pendulous frequency n=1,2,3, i.e., three counted are measured three times
It is respectively N that distinct pulse widths, which count,11、N21、N31, N12、N22、N32, N13、N23、N33;
3. the radiation dose rate measured in the known reference instrument three times is respectively H1、H2、H3, measure system three times by described in
The step-by-step counting N corresponding to three section pulsewidths counted out1n、N2n、N3nSubstitution formula Hn=N1n*Y1+N2n*Y2+N3n*Y3In, composition
The reference radiation calibration factor Y to be measured corresponding to these three pulsewidth sections is obtained in ternary linear function groupt, wherein three pulsewidths
Section t=1,2,3, ternary linear function group is as follows:
Ternary linear function group is solved,
4. in unit measuring section T, pulse corresponding to three pulsewidth sections in statistics scintillator detector instrument is measured
Count N1、N2、N3;
5. by required radiometric calibration factor Y in 3.1、Y2、Y34. in the three pulsewidth sections counted are measured in instrument to be measured
Corresponding step-by-step counting N1、N2、N3Substitution formula H*=N1*Y1+N2*Y2+N3*Y3In, you can scintillator detector is obtained and treats dose
Rate H*。
2. it is based on scintillator detector dosage rate detection method according to claim 1, it is characterised in that:When unit measures
Between in section T, the pulse width section measured by scintillator detector is not limited to be divided into three sections, can also be according to different flickers
The actual pulse signal width feature that body and radiation detection intensity-conversion go out is divided;Wherein pulses of radiation width section hop count
What is divided is more, then corresponding required reference radiation calibration factor number is more, then scintillator detector radiation dose rate
Measured value it is more accurate.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201810209495.7A CN108196293B (en) | 2018-03-14 | 2018-03-14 | One kind being based on scintillator detector dosage rate detection method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201810209495.7A CN108196293B (en) | 2018-03-14 | 2018-03-14 | One kind being based on scintillator detector dosage rate detection method |
Publications (2)
Publication Number | Publication Date |
---|---|
CN108196293A true CN108196293A (en) | 2018-06-22 |
CN108196293B CN108196293B (en) | 2019-01-15 |
Family
ID=62595757
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201810209495.7A Active CN108196293B (en) | 2018-03-14 | 2018-03-14 | One kind being based on scintillator detector dosage rate detection method |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN108196293B (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110456402A (en) * | 2019-07-22 | 2019-11-15 | 北京云端光科技术有限公司 | Dose of radiation detection method and device |
Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2004108796A (en) * | 2002-09-13 | 2004-04-08 | Aloka Co Ltd | Radiation measurement device |
WO2010017218A2 (en) * | 2008-08-06 | 2010-02-11 | Mirion Technologies (Gds), Inc. (Formerly Known As Global Dosimetry Solutions, Inc.) | Method and apparatus to discriminate out interference in radiation dosage measurements |
CN105137469A (en) * | 2015-06-03 | 2015-12-09 | 南京航空航天大学 | Radioactive detection system and radioactive detection method |
CN205507100U (en) * | 2015-12-14 | 2016-08-24 | 上海怡星机电设备有限公司 | Environment X, gamma dose rate measuring apparatu |
CN106094002A (en) * | 2016-07-28 | 2016-11-09 | 中国船舶重工集团公司第七〇九研究所 | A kind of Miniature Buoy formula water body region gamma activity monitor |
CN106125122A (en) * | 2016-06-13 | 2016-11-16 | 成都新核泰科科技有限公司 | Highfield radiation detecting system |
CN106873019A (en) * | 2017-01-06 | 2017-06-20 | 中国科学院高能物理研究所 | A kind of radiation dose measurement method |
CN107526094A (en) * | 2016-06-21 | 2017-12-29 | 纪新辉 | A kind of modified scintillator detector signal processing circuit |
CN107643538A (en) * | 2017-10-18 | 2018-01-30 | 中国检验检疫科学研究院 | A kind of device for being used to verify scintillator detector performance |
-
2018
- 2018-03-14 CN CN201810209495.7A patent/CN108196293B/en active Active
Patent Citations (9)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2004108796A (en) * | 2002-09-13 | 2004-04-08 | Aloka Co Ltd | Radiation measurement device |
WO2010017218A2 (en) * | 2008-08-06 | 2010-02-11 | Mirion Technologies (Gds), Inc. (Formerly Known As Global Dosimetry Solutions, Inc.) | Method and apparatus to discriminate out interference in radiation dosage measurements |
CN105137469A (en) * | 2015-06-03 | 2015-12-09 | 南京航空航天大学 | Radioactive detection system and radioactive detection method |
CN205507100U (en) * | 2015-12-14 | 2016-08-24 | 上海怡星机电设备有限公司 | Environment X, gamma dose rate measuring apparatu |
CN106125122A (en) * | 2016-06-13 | 2016-11-16 | 成都新核泰科科技有限公司 | Highfield radiation detecting system |
CN107526094A (en) * | 2016-06-21 | 2017-12-29 | 纪新辉 | A kind of modified scintillator detector signal processing circuit |
CN106094002A (en) * | 2016-07-28 | 2016-11-09 | 中国船舶重工集团公司第七〇九研究所 | A kind of Miniature Buoy formula water body region gamma activity monitor |
CN106873019A (en) * | 2017-01-06 | 2017-06-20 | 中国科学院高能物理研究所 | A kind of radiation dose measurement method |
CN107643538A (en) * | 2017-10-18 | 2018-01-30 | 中国检验检疫科学研究院 | A kind of device for being used to verify scintillator detector performance |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110456402A (en) * | 2019-07-22 | 2019-11-15 | 北京云端光科技术有限公司 | Dose of radiation detection method and device |
CN110456402B (en) * | 2019-07-22 | 2021-09-10 | 北京云端光科技术有限公司 | Radiation dose detection method and device |
Also Published As
Publication number | Publication date |
---|---|
CN108196293B (en) | 2019-01-15 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JP3958069B2 (en) | Radiation measurement equipment | |
US9945965B2 (en) | Universal readout for silicon photomultiplier based detectors | |
US9910167B2 (en) | Method for digitalizing scintillation pulse | |
US7592596B2 (en) | Methods and systems for medical imaging | |
CN109581461B (en) | Nuclear pulse energy measuring method and system | |
RU2009108306A (en) | DEVICE AND METHOD FOR SPECTRAL COMPUTER TOMOGRAPHY | |
JP2011519415A (en) | Radiation imaging using individual signal resolution | |
US20020145115A1 (en) | Readout circuit for a charge detector | |
Jie et al. | Energy calibration of a BC501A liquid scintillator using a γ-γ coincidence technique | |
CN107247284A (en) | The gain correcting device and method of a kind of scintillation detector | |
JP2012013563A (en) | Radiation measuring apparatus | |
US7511264B2 (en) | Method of resolving ambiguity in photon counting-based detectors | |
CN114252900A (en) | Counting activity meter for measuring activity of radioactive source | |
JP2004108796A (en) | Radiation measurement device | |
CN108196293B (en) | One kind being based on scintillator detector dosage rate detection method | |
JP2003513250A (en) | Difference correction method and difference correction device | |
CN109507716A (en) | A method of obtaining scintillator detector energy information | |
US10031239B2 (en) | Method for measuring dosage by means of a radiation detector, especially an X-radiation or gamma-radiation detector, used in the spectroscopic mode, and dosage measurement system using said method | |
CN109031388A (en) | Radon consistence absolute measuring system and method in a kind of water | |
JP4893950B2 (en) | Radioactivity absolute measurement method, radiation detector assembly detection efficiency determination method, and radiation measurement apparatus calibration method | |
CN109581468B (en) | Method for identifying weak gamma radioactive source under environmental background | |
JP4417972B2 (en) | Radiation measurement equipment | |
JPH01134291A (en) | Scintillation type dose rate meter | |
TW201040570A (en) | Method and apparatus of all function environmental gamma radiation monitor | |
Reardon et al. | Neutron Capture Gamma-Rays in Cadmium, Cobalt, and Chlorine |
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 | ||
CB02 | Change of applicant information | ||
CB02 | Change of applicant information |
Address after: 330096 No. 900 Gaoxin Avenue, Nanchang City, Jiangxi Province Applicant after: Zhongguang Nuclear Beigu Technology Co., Ltd. Address before: 330096 No. 900 Gaoxin Avenue, Nanchang City, Jiangxi Province Applicant before: Cnpec kaidani Polytron Technologies Inc |
|
GR01 | Patent grant | ||
GR01 | Patent grant |