GB/T 30151-2013Characterization of the spectrum background in HP Ge gamma-ray spectrometry (English PDF)
高纯锗γ谱仪本底谱的特性
This is a limited preview
Buy now to download the full PDF (10 pages)
Need quotation for your management?
Get a formal quotation for GB/T 30151-2013 in 30 minutes.
Issued by
Standardization Administration of China
Level / Type
National · Recommended
Issue date
December 17, 2013
Implementation date
August 1, 2014
Scope
GB/T 30151-2013 is the English-translated version of 高纯锗γ谱仪本底谱的特性.
GB/T 30151-2013 — This standard specifies the gamma spectrometer with high purity germanium detector consisting of the background spectrum characteristics.
This standard applies to the high-purity germanium detector gamma spectrometer consisting of the acquisition of the background spectrum, particularly low background detectors capture the background spectrum. This standard does not address methods to reduce background.
Found what you need?
Document preview — GB/T 30151-2013
National Standard of the People's Republic of China
- ICS
- 27.120
- Classification
- F 81
Issued by: Standardization Administration of China
Contents
- Preface
- Introduction
- 1 Scope
- 2 Normative references
- 3 Terms and definitions
- Description 4 Spectrum
- 5 Bottom spectral characteristics
- Appendix A (informative) common peak energy
- Illustrative examples and Annex B (informative) background continuous spectrum and the background peak measured
- Reference
Foreword
This standard was drafted in accordance with GB/T 1.1-2009 given rules.
This standard uses redrafted law revision adopted IEC 61976:2000 special "high purity germanium spectrometer instrument nuclear gamma-ray spectrometer spectrum of the background Sex. " the standard IEC 61976:2000 The main changes are as follows [terms of these modifications have been involved in the blank position by its outer margins A single vertical line (|) be indicated].
--- Increasing the "Introduction" to include purposes other "Scope and purpose" in the standard preparation of IEC standards related to the content of Chapter 1;
--- According to GB/T 1.1 requirement to rewrite Chapter 1, "scope";
--- Chapter 2, "Normative references", with GB/T 4960.6-2008 "Nuclear Science and Technology - Part 6. Nuclear Instrumentation" in place (see IEC 60050-393:2003 and IEC 60050-394:2007 preparation) IEC 60050-393:1996 "Nuclear Instruments Physical phenomena and basic concepts "and IEC 60050-394:1995" Nuclear Instruments Instruments "; increased references GB/T 4833.1 "Multi-channel analyzer - Part 1. Technical requirements and test methods" and GB/T 7167 "germanium gamma-ray detector test side law";
--- Change the title of Chapter 3 "Terms and Definitions";
--- Chapter 4, "the description of the spectrum" to increase the general measurement gamma spectrum, namely "HPGe gamma spectrometer gamma spectrum should adopt the general measurement GB/Method "T 4833.1 and GB/T 7167 provided;
--- 5.1 "background continuous spectrum" "(also determine energy in any other interested)" with "(also in any other interested Point energy or energy interval determined) "to expand the background continuous spectrum measured energy range of options;
--- In 5.2 "contains the total number of tracks," add "error is relatively small and the calculation results of the measurements, it may be necessary an increase in the "first and" on. ";
--- Increase in Table A.1 Notes to Table. "The 226Ra, 226Ra and 222Rn under equilibrium conditions can be measured 226Ra spectrum; for 238U, 238U and 226Ra under equilibrium conditions (difficult to achieve) can be obtained by measuring the spectrum of 238U and 226Ra analysis and calculation of Spectrum. ";
--- Increase in Appendix B (informative) "illustrative examples of the bottom and continuous spectrum measurements of peak and background", that is, for Chapter 5, "this Detroit "Of the formula (1) and (2) gives a schematic view, in order to deepen the understanding of the formula, it has added two solid background continuous spectrum and background peaks Measured spectra, in order to enrich the content of this standard;
--- Increased references included in the GB/T 2900.81-2008 "Electrotechnical Terminology Nuclear Instruments Physical phenomena and basic concepts" and GB/T 2900.82-2008 "Electrotechnical Terminology nuclear instrumentation, systems, equipment and detectors." this standard by the National Nuclear Instrument Standardization Technical Committee (SAC/TC30) centralized.
This standard was drafted. Nuclear Industry Standardization Institute, Chinese Academy of Sciences Institute of High Energy Physics, Tsinghua University.
Introduction
The purpose of this standard is to describe and measure the high-purity germanium detector composed of gamma spectrometer background spectrum to provide a unified approach and its definition the method is particularly suitable for low background gamma spectrometer Review by HPGe detector configuration.
Measurement methods defined in this standard background continuous spectrum and the background peak is determined on the basis of a large number of experimental results, this method not only mention Supply manufacturers and users, but also provide a similar comparison between the measurement of several different types of high-purity germanium detector.
Background HPGe gamma Spectrometer Spectral characteristics
1 Scope
This standard specifies the gamma spectrometer with high purity germanium detector consisting of the background spectrum characteristics.
This standard applies to the high-purity germanium detector gamma spectrometer consisting of the acquisition of the background spectrum, particularly low background detectors capture the background spectrum.
This standard does not address methods to reduce background.
2 Normative references
The following documents for the application of this document is essential. For dated references, only the dated version suitable for use herein Member. For undated references, the latest edition (including any amendments) applies to this document.
GB/T 4833.1 multi-channel analyzer - Part 1. Technical requirements and test methods (GB/T 4833.1-2007, IEC 61342:1995, MOD) GB/T 4960.6 nuclear science and technology - Part 6. Nuclear instrumentation GB/T 7167 germanium gamma-ray detector test methods
3 Terms and Definitions
GB/T 4960.6 and define the following terms and definitions apply to this document.
(Ionizing radiation) spectrum (ofanionizingradiation) Usually it refers to with energy distribution, such as the relationship between particle emission rate and its energy value of a particular amount of radiation.
[GB/T 4960.6-2008,3.1.37] 3.2 FWHM fulwidthathalfmaximum; FWHM Single peak in the distribution curve formed from the horizontal axis between two points on the curve at half peak.
[GB/T 4960.6-2008,3.2.27] 3.3 Sample Attention and need to measure a material in which the radionuclide and content.
External background in the absence of the sample in a given configuration, high-purity germanium detector measured spectrum.
Samples induced background sample-inducedbackground Emitted by the sample, and does not include all the spectral data detector placed near any source (including samples) of all-round peak.
Total background External background and the background of the sample and induced.
The bottom peak backgroundpeak all-around peaks generated by an external source of any of the background spectrum.
Background continuum External background spectrum does not belong to any data Almighty peak.
Peak baseline Near the end of the peak region that belongs to the external background and not part of the sample induced by the almighty bottom peak count.
4 Description, Spectrum
The bottom spectrum collection time should be long enough to ensure that the energy within the range of one standard deviation 100keV statistical uncertainty about 5%. This means that, in the area of \u200b\u200benergy 100keV measured spectra, counts per channel should not be less than 400 to reduce the statistical uncertainty in the data Given the degree of impact on the bottom spectrum measurements. Mean number of spectrum should be more than enough, that is, the energy range of interest collected per channel energy representation foot Small enough so that, by - a calculation error "channel energy" transformation caused by the uncertainty compared with the theoretical value small enough.
Before you begin measuring the background spectrum, shall take all necessary precautions to avoid possible in laboratory experiments, inspection, calibration using any source of radiation to which (including natural and artificial, such as X-ray, neutron generators and particle accelerators) on the measured background spectrum.
External factors that can seriously affect the background spectrum is.
Geometrical position a) measurement;
b) shielding material and its thickness and geometry (including the probe position);
Date and time c) measurement;
d) measurement of weather conditions;
Duration e) measurement;
f) airborne radioactivity;
g) the circulation of air in the measuring chamber.
Therefore, a detailed description of the measurement location and condition [above a) ~ g)] should be included in the measurement results of the report.
HPGe gamma spectrometer general measurement gamma spectrum should adopt the method of GB/T 4833.1 provides and GB/T 7167.
Peak energy commonly used radionuclides in Appendix A.
5 Bottom spectral characteristics
5.1 Bottom continuous spectrum
Background continuum average of B (E) to the "counts per keV one thousand seconds" said. B (E) should be counted within the following range of energy level Mean, that is designated as the center of energy, which is the width of the detector in a given FWHM energy (energy resolution) five times. In all calculations the number of tracks from the energy to the conversion should be rounded (ie decimal between 0.0 and 0.49999 accrued to 0.0, between 0.5 and 0.99999 Decimal accrued 1.0).
B (E) by the formula (1) is given by.
5F (E) 1
· sum
j 2.5F (E)
i = j-2.5F (E)
Ci (1)
Where.
B (E) --- the average background continuous spectrum at energy E, in units of counts per keV one thousand seconds (keV × 1000s) -1;
TL --- live time, in seconds (s);
G --- channel number conversion factor to energy, in units of keV per channel (channel/keV);
F (E) --- detector at energy E of the resolution of the unit is to half width (FWHM) represents the number of channels;
Ci --- i-channel track count;
j --- corresponds to the number of road energy E.
The average amount of B (E) represents the continuous spectrum of the background, a description of the background spectrum without background peak areas most useful. It also describes the background peak region Average background, but it can mask the true value of the individual peaks. For a particular high purity germanium detectors, B (E) is preferably at three energy points (50keV, 140keV and 1350keV) determine (section may also determine at any other energy or energy point of interest), and the result Recorded in the background spectrum measurement reports.
And illustrative examples of the bottom continuous spectrum measurements in Appendix B.
5.2 Bottom peak
In the external background spectrum, the final version of the end of the peak energy of the selected net peak area ANP (E) to "count per thousand second" representation. ANP (E) to the selected Energy at three times the FWHM area totaled minus peaks baseline counts the same area calculated. Peak baseline counts by the energy region below the background peak Count count is higher than the domain of this region and the end of the peak energy is determined. Lower than the peak energy of the background region from less than 3 times the background peak energy FWHM extended to 1.5 times the FWHM. Above background peak area from the peaks above background energy of 1.5 times FWHM extended to three times the FWHM.
ANP (E) by the formula (2) is given by.
ANP (E) =
T [L sum
j 1.5F (E)
i = j-1.5F (E)
Ci- sum
j-1-1.5F (E)
i = j-1-3F (E)
Ci- sum
j 1 3F (E)
i = j 1 1.5F (E)
C] i (2)
Where.
ANP (E) --- corresponds to the net area of \u200b\u200bthe bottom peak energy E per unit time, measured in counts per one thousand seconds (1/1000s).
When the ANP (E) is negative should be reported as zero.
When using the formula (2), such that "first and" equal to the number of channels included in the "second and" and "the third and the" total number of channels included, and the calculation results of the measurement error is relatively small, it may need to increase in a "first and" on. If you observe a baseline Distinct slopes, the second and the third and the number of channels should be equal. It is necessary to more than three normalization is contained in each summation term the number of channels in order to correctly calculate the number of channels.
And illustrative examples of the bottom peak measured in Appendix B.
Appendix A
(Informative)
Common peak energy
The following peak energy from natural and artificial radionuclides emitted radioactive material approved by the presence of the detector or the natural environment, and many users are interested in Table A.1. For specific applications, but also the provisions of other isotopes and energy. "Yu [universe] born [into] the" it means cosmic rays interacting with the listed material generated.
Note. Health-interaction data from "low-activation analysis background gamma ray analysis laboratory", RMLindstrom, DJLindstrom, LASlaback and JKLangland, Nuclear Instruments and Methods (NIM) A299 (1990) 425 ~ 429.
Table A.1 common gamma-ray peak energy meters
Energy/keV energy source/keV energy source/keV source
13 UX ray 185.7,186.2 238U, 226Raa 846.8 universe 56Fe
25.6 231Th (235U) 197.1 universe 71Ge, 19F 911.1 228Ac (232Th) 31.8 ~ 37.3 137Cs 215.5 universe 77Gem 962.1 universe 63Cu 46.5 210Pb (238U) 238.6 212Pb (232Th) 968.9 228Ac (232Th)
53.4 Yu students 73Gem 295.2 214Pb (238U) 1001.0 234mPa (238U)
59.5 241Am 351.9 214Pb (238U) 1063.6 cosmogenic of 207Pb 63.3 234Th (238U) 511 cosmogenic, the annihilation of the cosmogenic 1115.5 65Cu Students 73Gem 569.7 66.7 Yu Yu students 207Pb 1120.3 214Bi (238U)
72.8 PbX ray 583.1 208Tl (232Th) 1173.2 60Co
75.0 PbX ray of 596.1 cosmogenic 74Ge (n, n ') 1238.1 214Bi (238U)
84.8 PbX ray 609.3 214Bi (238U) 1327.0 cosmogenic of 63Cu
87.3 PbX ray 661.6 137Cs 1332.5 60Co
92.6 234Th (238U) 669.6 cosmogenic of cosmogenic of 63Cu 63Cu 1412.1 Students 19F 693.4 109.9 Yu Yu students 72Ge (n, n ') 1460.8 40K
122.1 Cosmogenic of 57Fe 727.2 212Bi (232Th) 1481.8 cosmogenic of 65Cu
139.7 Cosmogenic of 75Gem 766.6 234mPa (238U) 1764.5 214Bi (238U) Students 77Gem 770.6 159.7 Yu Yu students 63Cu 2614.6 208Tl (232Th) Students 71Ge 803.3 174.9 Yu Yu students 206Pb (n, n ') Note. 226Ra, 226Ra and 222Rn under equilibrium conditions can be measured 226Ra spectrum; for 238U, 238U and 226Ra under equilibrium conditions (difficult to achieve) can by measuring and analyzing the spectrum obtained 238U and 226Ra computing spectrum.
......
This preview omits tables, figures, formulas and parts of the technical clauses. The complete document — 10 pages — is available in the English PDF.
Referenced standards
Normative references
- GB/T 4833.1Multichannel analyzers - Part 1: Technical requirements and test methods for pulse amplitude analysis
- GB/T 4833.1-2007Multichannel analyzers - Part 1: Technical requirements and test methods for pulse amplitude analysis
- GB/T 4960.6Glossary of terms: nuclear science and technology - Nuclear instrumentation
- GB/T 7167Test procedures for germanium gamma-ray detectors
IEC 61342
How to Download GB/T 30151-2013
- 1
Add to cart
Click "Download PDF" on this page and choose "Buy this standard". You can add more standards before checkout.
- 2
Checkout
Enter your email and billing details. Payment is processed securely by Stripe (cards or bank transfer). Prefer bank details? Request a quotation (min. order $300).
- 3
Instant delivery (0–9 sec)
Delivery is automatic: within seconds of payment you'll receive an email with a secure download link. The link stays valid for 72 hours.
- 4
Invoice included
A tax invoice is attached to the confirmation email. Need a custom invoice? Contact us.
Related Standards
GB/T 4833.1-2025 — Multichannel analyzers - Part 1: Technical requirements and test methods for pulse amplitude analysis
GB/T 4960.6-2008 — Glossary of terms: nuclear science and technology - Nuclear instrumentation
GB/T 7167-2008 — Test procedures for germanium gamma-ray detectors
Secure payment via Stripe
Payments accepted
GB/T 30151-2013
$195.00