Practical method for experimental effective atomic number in the coherent to Compton scattering ratio

ArticleAçık Erişim

Özet

A practical method of calculating Zeff was developed for the coherent to Compton scattering ratio and the method is applicable for any material with known weight percentages of different elements in the compound. The coherent to Compton scattering ratio depends only on the mixture under study and provides a measurement of certain complicated functions of the atomic number Z and Zeff. In order to measure the effective atomic number of Sb2O3, BaO, La2O3, CeO2 and Nd2O3, the linear differential scattering coefficients of 59.5 keV γ-rays have been studied using a high-resolution Si(Li) semi-conductor detector. The coherent to Compton scattering ratio R is taken from the linear differential scattering coefficients μ(E, q). The results obtained have been compared with relativistic (RT) and non-relativistic (NRT) theoretical values. © 2005 Elsevier Ltd. All rights reserved.

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RDL Kalıcı Bağlantı (PID)
https://rdlopen.rawdatalibrary.net/r/ebyu/16060Resmi atıflarda kullanılan kalıcı adres
DOI
https://doi.org/10.1016/j.jqsrt.2005.11.014Yayıncı resmi DOI adresi
Tam Kayıt
AlanDeğerDil
dc.contributor.authorIçelli, Orhan
dc.date.accessioned2026-10-18T20:30:53.612489642Z
dc.date.available2026-10-18T20:30:53.612489642Z
dc.date.issued2006
dc.description.abstractA practical method of calculating Zeff was developed for the coherent to Compton scattering ratio and the method is applicable for any material with known weight percentages of different elements in the compound. The coherent to Compton scattering ratio depends only on the mixture under study and provides a measurement of certain complicated functions of the atomic number Z and Zeff. In order to measure the effective atomic number of Sb2O3, BaO, La2O3, CeO2 and Nd2O3, the linear differential scattering coefficients of 59.5 keV γ-rays have been studied using a high-resolution Si(Li) semi-conductor detector. The coherent to Compton scattering ratio R is taken from the linear differential scattering coefficients μ(E, q). The results obtained have been compared with relativistic (RT) and non-relativistic (NRT) theoretical values. © 2005 Elsevier Ltd. All rights reserved.
dc.identifier.doi10.1016/j.jqsrt.2005.11.014
dc.identifier.endpage158
dc.identifier.issn0022-4073
dc.identifier.issue1
dc.identifier.scopus2-s2.0-33747668905
dc.identifier.startpage151
dc.identifier.urihttps://rdlopen.rawdatalibrary.net/r/ebyu/16060
dc.identifier.volume101
dc.language.isoen
dc.publisherElsevier Ltd
dc.relation.ispartofJournal of Quantitative Spectroscopy and Radiative Transfer
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectCompton and coherent scattering
dc.subjectPhoton transport
dc.subjectRadioactive materials
dc.subjectX-ray fluorescence spectrometry
dc.subjectCoherent light
dc.subjectFluorescence
dc.subjectHigh resolution electron microscopy
dc.subjectPhotons
dc.subjectX ray spectrometers
dc.subjectCompton scattering ratio
dc.subjectLinear differential scattering coefficients
dc.subjectlight scattering
dc.subjectX-ray fluorescence
dc.subjectScattering
dc.titlePractical method for experimental effective atomic number in the coherent to Compton scattering ratio
dc.typeArticle
dspace.entity.typePublication
rdl.citation.scopus37
rdl.source.indexSCOPUS