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本文(ANSI N42.12-1994 Calibration and Usage of Thallium-Activated Sodium Iodide Detector Systems for Assay of Radionuclides《铊的校准和使用.放射性核素分析用活性碘化钠探测系统》.pdf)为本站会员(brainfellow396)主动上传,麦多课文库仅提供信息存储空间,仅对用户上传内容的表现方式做保护处理,对上载内容本身不做任何修改或编辑。 若此文所含内容侵犯了您的版权或隐私,请立即通知麦多课文库(发送邮件至master@mydoc123.com或直接QQ联系客服),我们立即给予删除!

ANSI N42.12-1994 Calibration and Usage of Thallium-Activated Sodium Iodide Detector Systems for Assay of Radionuclides《铊的校准和使用.放射性核素分析用活性碘化钠探测系统》.pdf

1、The Institute of Electrical and Electronics Engineers, Inc.3 Park Avenue, New York, NY 10016-5997, USACopyright 1995 by the Institute of Electrical and Electronics Engineers, Inc.All rights reserved. Published1995. Printed in the United States of America.IEEE is a registered trademark in the U.S. Pa

2、tent the assay for radioactivity; and thedetermination of gamma ray energies and intensities are established. Both energy calibration andefficiency calibration are coveredKeywords: calibration, efficiency calibration, energy calibration, gamma-ray energy, radioactivity,radionuclidesCopyright The Ins

3、titute of Electrical and Electronics Engineers, Inc. Provided by IHS under license with IEEENot for ResaleNo reproduction or networking permitted without license from IHS-,-,-IEEE Standardsdocuments are developed within the Technical Committees of theIEEE Societies and the Standards Coordinating Com

4、mittees of the IEEE StandardsBoard. Members of the committees serve voluntarily and without compensation.They are not necessarily members of the Institute. The standards developed withinIEEE represent a consensus of the broad expertise on the subject within the Instituteas well as those activities o

5、utside of IEEE that have expressed an interest in partici-pating in the development of the standard.Use of an IEEE Standard is wholly voluntary. The existence of an IEEE Standarddoes not imply that there are no other ways to produce, test, measure, purchase, mar-ket, or provide other goods and servi

6、ces related to the scope of the IEEE Standard.Furthermore, the viewpoint expressed at the time a standard is approved and issued issubject to change brought about through developments in the state of the art and com-ments received from users of the standard. Every IEEE Standard is subjected toreview

7、 at least every five years for revision or reaffirmation. When a document ismore than five years old and has not been reaffirmed, it is reasonable to conclude thatits contents, although still of some value, do not wholly reflect the present state of theart. Users are cautioned to check to determine

8、that they have the latest edition of anyIEEE Standard.Comments for revision of IEEE Standards are welcome from any interested party,regardless of membership affiliation with IEEE. Suggestions for changes in docu-ments should be in the form of a proposed change of text, together with appropriatesuppo

9、rting comments.Interpretations: Occasionally questions may arise regarding the meaning of portionsof standards as they relate to specific applications. When the need for interpretationsis brought to the attention of IEEE, the Institute will initiate action to prepare appro-priate responses. Since IE

10、EE Standards represent a consensus of all concerned inter-ests, it is important to ensure that any interpretation has also received the concurrenceof a balance of interests. For this reason IEEE and the members of its technical com-mittees are not able to provide an instant response to interpretatio

11、n requests except inthose cases where the matter has previously received formal consideration. Comments on standards and requests for interpretations should be addressed to:Secretary, IEEE Standards Board445 Hoes LaneP.O. Box 1331Piscataway, NJ 08855-1331USAIEEE Standards documents may involve the u

12、se of patented technology. Theirapproval by the Institute of Electrical and Electronics Engineers does not mean thatusing such technology for the purpose of conforming to such standards is authorizedby the patent owner. It is the obligation of the user of such technology to obtain allnecessary permi

13、ssions.Copyright The Institute of Electrical and Electronics Engineers, Inc. Provided by IHS under license with IEEENot for ResaleNo reproduction or networking permitted without license from IHS-,-,-iiiIntroduction(This introduction is not a part of ANSI N42.12-1994, American National Standard Calib

14、ration and Usage of Thallium-Activated Sodium Iodide Detector Systems for Assay of Radionuclides.)This standard, a revision of ANSI N42.12-1980, is the responsibility of the Accredited Standards CommitteeN42 on Radiation Instrumentation. Committee N42 delegated the development of this standard to it

15、s Sub-committee N42.2. Drafts were reviewed by Committee N42, Subcommittee N42.RM on Radioactivity Mea-surements, and other interested parties, and the comments received were utilized in producing the standardas finally approved. The standard was approved by N42 letter ballot of 11 April 1994.At the

16、 time it approved this standard, the Accredited Standards Committee on Radiation Instrumentation,N42, had the following members:Louis Costrell,ChairLuigi Napoli,Administrative SecretaryOrganization Represented Name of RepresentativeAmerican Conference of Governmental Industrial HygienistsJesse Liebe

17、rmanHealth Physics Society.George CampbellJoseph R. Stencel (Alt.)Institute of Electrical and Electronics Engineers.Louis CostrellJulian Forster (Alt.)Anthony J. Spurgin (Alt.)Lawrence Berkeley LaboratoryEdward J. LampoLawrence Livermore National Laboratory.Paul L. PhelpsNational Institute of Standa

18、rds and TechnologyLouis CostrellMichael P. Unterweger (Alt.)Oak Ridge National Laboratory.Hugh R. BrashearPacific Northwest LaboratoriesKenneth L. SwinthUS Army Center for EW/RSTA.Edward GroeberUS Department of EnergyGerald GoldsteinUS Federal Emergency Management Agency .Carl R. SiebentrittUS Nucle

19、ar Regulatory Commission.Edward C. Wenzinger, Sr.Members-at-LargeJoseph C. BellianErnesto A. CorteMorgan CoxJohn M. GallagherJack M. SelbyAl N. TschaecheEdward J. VallarioLee J. WagnerSanford Wagner At the time this standard was approved, Subcommittee N42.RM had the following members: Frank X. Masse

20、,ChairJ. M. R. Hutchinson,SecretaryRobert Ayres Bert M. Coursey Y. KobyashiJoseph G. Bellian Michael Devine David McCurdyJohn D. Buchanan Roger Ferris D. M. MontgomeryR. F. Coley Robert J. Gehrke Carl W. SeidelCopyright The Institute of Electrical and Electronics Engineers, Inc. Provided by IHS unde

21、r license with IEEENot for ResaleNo reproduction or networking permitted without license from IHS-,-,-ivThe working group for this standard had the following members:Joseph G. Bellian,Project LeaderRod Dayton Tom Jenkins Robert KinzerJ. M. R. Hutchinson Peter Paul Ernesto A. CorteMelvyn Halbert Don

22、W. Miller Frank X. Massey The following persons were on the balloting committee:Joseph G. Bellian Gerald Goldstein Anthony J. SpurginHugh R. Brashear Edward Groeber Joseph R. StencilGeorge Campbell Edward J. Lampo Kenneth L. SwinthErnesto A. Corte Jesse Lieberman Al N. TschaecheLouis Costrell Paul L

23、. Phelps Michael UnterwegerMorgan Cox Jack M. Selby Edward J. VallarioJulian Forster Carl L. Siebentritt Sanford WagnerJohn M. Gallagher Edward C. Wenzinger, Sr.Mary Lynne NielsenIEEE Standards Project EditorCopyright The Institute of Electrical and Electronics Engineers, Inc. Provided by IHS under

24、license with IEEENot for ResaleNo reproduction or networking permitted without license from IHS-,-,-vContentsCLAUSE PAGE1. Overview 11.1 Scope 11.2 Purpose. 12. References 23. Definitions 24. Procedure . 34.1 Total spectrum counting systems. 34.2 SCA counting systems . 54.3 MCA counting systems 65.

25、Sources of systematic error 86. Precautions. 96.1 Assay for a radionuclide for which no radioactivity standard is readily available 96.2 Assay of mixtures of radionuclides 96.3 Thin-Window detectors . 96.4 Count rates . 96.5 Geometric correction factors 96.6 Counting statistics 96.7 Dead-Time correc

26、tions. 96.8 Correction for decay during the counting period. 106.9 Counting geometry. 116.10 Spectral features. 116.11 Full-Energy-Peak efficiency versus energy function or curve 116.12 Net count rate. 126.13 Temperature effects . 126.14 Linearity. 127. Bibliography 12Copyright The Institute of Elec

27、trical and Electronics Engineers, Inc. Provided by IHS under license with IEEENot for ResaleNo reproduction or networking permitted without license from IHS-,-,-Copyright The Institute of Electrical and Electronics Engineers, Inc. Provided by IHS under license with IEEENot for ResaleNo reproduction

28、or networking permitted without license from IHS-,-,-American National Standard Calibration and Usage of Thallium-Activated Sodium Iodide Detector Systems for Assay of Radionuclides1. Overview1.1 ScopeThis standard establishes methods for performance testing, calibration, and usage of thallium-activ

29、atedsodium iodide NaI(Tl) detector systems for the measurement of gamma ray emission rates of radionu-clides; the assay for radioactivity; and the determination of gamma ray energies and intensities. It coversboth energy calibration and efficiency calibration. The following three techniques are cons

30、idered:a) Total spectrum counting (see 4.1) employs a system that counts all pulses above a low-energythreshold (see 6.1, 6.2, and 6.3).b) Single-channel analyzer (SCA) counting (see 4.2) employs a system with a counting “window,”which establishes upper and lower energy boundaries (see 6.1, 6.2, and

31、 6.3).c) Multichannel analyzer (MCA) counting (see 4.3) employs a system in which multiple counting win-dows are utilized. This technique allows measurements for which the continuum under the full-energy peak may be subtracted without introducing unacceptable error.In case of overlapping peaks in th

32、e spectrum, it is realized that an MCA with access to a spectrum-strippingprogram is necessary. Such cases are not covered by this standard.1.2 PurposeThe purpose of this document is to provide a standardized basis for the calibration and usage of sodiumiodide detector systems for the measurement of

33、 gamma ray emission rates of radionuclides. Typical applica-tions include radionuclide identification and assay in various industrial, environmental, and medical applica-tions. An NaI(Tl) detector system consists of three major components: a scintillating medium that producesa flash of light when io

34、nizing radiation interacts with it; one or more photomultipliers, optically coupled tothe scintillator, which converts the light flash to an amplified electrical impulse; and associated electronicinstrumentation that powers the photomultiplier and processes the output signal. (See IEEE Std 398-1972.

35、1)1Information on the reference can be found in clause 2.1ANSIN42.12-1994 AMERICAN NATIONAL STANDARD CALIBRATION AND USAGE OF THALLIUM-ACTIVATEDCopyright The Institute of Electrical and Electronics Engineers, Inc. Provided by IHS under license with IEEENot for ResaleNo reproduction or networking per

36、mitted without license from IHS-,-,-The theory of operation of NaI(Tl) detectors is presented in numerous publications, including B3, B5,and B9 in clause 7.2. ReferencesThis standard shall be used in conjunction with the following publication:IEEE Std 398-1972 (Reaff 1990), IEEE Standard Test Proced

37、ures for Photomultipliers for ScintillationCounting and Glossary for Scintillation Counting Field (ANSI).23. Definitions3.1 accuracy: The degree of agreement of the measured value with the true value of the quantity beingmeasured.3.2 assay: The determination of the activity of a radionuclide in a sa

38、mple.3.3 ambient background: Those counts that can be observed, and thereby allowed for, by measuring a sam-ple that is identical to the unknown sample in all respects except for the absence of radioactivity. Thesecounts are attributable to environmental radioactivity in the detector itself, the det

39、ector shielding material,and the sample container; cosmic rays; electronic noise pulses; etc.3.4 check source: A radioactive source, not necessarily calibrated, that is used to confirm the continuing sat-isfactory operation of an instrument.3.5 correlated gamma ray summing: The simultaneous detectio

40、n of two or more gamma rays originatingfrom a single atom disintegration.3.6 dead time (td): The time after a triggering pulse during which the system is unable to retrigger.3.7 efficiency: The net number of counts registered by the detector system per unit of time, divided by thenumber of photons o

41、f interest originating in the radioactive source during the same unit of time.3.8 energy calibration: The relationship between the height of the amplifier output pulse and the energy ofthe photons originating in the radioactive source.3.9 full-energy peak: The peak in a pulse height spectrum that co

42、rresponds to total absorption of a gammaphoton in the NaI(Tl) detector.3.10 full width at half maximum (FWHM): The full width of a gamma photon peak distribution measuredat an ordinate halfway between the maximum ordinate of the peak and the background.3.11 live time: The total time of the measureme

43、nt minus the total dead time.3.12 precision: The degree of agreement of repeated measurements of the same property, expressed quanti-tatively as the standard deviation computed from the results of the series of measurements.3.13 pulse height radiation: See 3.16.2IEEE publications are available from

44、the Institute of Electrical and Electronics Engineers, 445 Hoes Lane, P.O. Box 1331, Piscataway,NJ 08855-1331, USA.2ANSISODIUM IODIDE DETECTOR SYSTEMS FOR ASSAY OF RADIONUCLIDES N42.12-1994Copyright The Institute of Electrical and Electronics Engineers, Inc. Provided by IHS under license with IEEENo

45、t for ResaleNo reproduction or networking permitted without license from IHS-,-,-3.14 radioactivity standard source: A radioactivity standard, as used in this document, shall be either aradioactivity standard that has been certified as to absolute radioactivity by a laboratory recognized as theNatio

46、nal Standardizing Laboratory of a country for radioactivity measurements or a radioactivity standardthat has been obtained from a supplier who participates in measurement assurance activities with theNational Standardizing Laboratory when such standards are available. In such measurement assurance a

47、ctiv-ities, the radioactivity calibration value of the suppliers should agree with the National Standardizing Labo-ratory value within the overall uncertainty stated by the supplier in its certification of the same batch ofsources or in its certification of similar sources.3.15 random photon summing

48、: The simultaneous detection of two or more photons originating from thedisintegrations of more than one atom.3.16 resolution, pulse height: The measured FWHM, after ambient background subtraction, of a gamma-ray peak distribution, expressed as a percentage of the pulse height corresponding to the c

49、entroid of the dis-tribution.3.17 sensitivity response: The net number of counts registered by the detector system per unit of time,divided by the activity of the radionuclide.3.18 shall: A verb indicating an action required by this standard.3.19 should: A verb indicating an action that is to be included when practical.3.20 simulated source: A radioactive source consisting of one or more long-lived radionuclid

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