Yayın:
The effect of the housing material on the NaI(Tl) detector response function

Basit Görünüm
dc.contributor.authorGurler, Orhan
dc.contributor.authorYalcin, S.
dc.contributor.authorOzmutlu, E. N.
dc.contributor.authorTarim, U. Akar
dc.date.accessioned2026-01-02T20:06:21Z
dc.date.issued2012-03-10
dc.description.abstractIn this study, a Monte Carlo program has been developed to simulate the response function of the NaI(Tl) detector with all features for 60Co and 137Cs and to investigate the effects of detector housing material on response function. The pulse height spectra in a 2″ × 2″ NaI(Tl) detector due to these gamma ray sources have been measured. Comparison of the experimentally obtained and simulated spectra shows that there is good agreement between both spectra. Energy distributions of gamma photons that generate the backscattering peak in the response function were obtained and the contribution of single, double and multiple Compton scattering events to these distributions was investigated.
dc.description.urihttps://doi.org/10.1007/s10967-012-1716-z
dc.description.urihttps://dx.doi.org/10.1007/s10967-012-1716-z
dc.description.urihttps://avesis.uludag.edu.tr/publication/details/c2f84dbd-4561-4df2-a66c-501da7d5a7c7/oai
dc.identifier.doi10.1007/s10967-012-1716-z
dc.identifier.eissn1588-2780
dc.identifier.endpage429
dc.identifier.issn0236-5731
dc.identifier.openairedoi_dedup___::538fcb6a7914e0746138e37ee624a3c1
dc.identifier.orcid0000-0001-6779-9230
dc.identifier.scopus2-s2.0-84862179446
dc.identifier.startpage425
dc.identifier.urihttps://hdl.handle.net/20.500.12597/35581
dc.identifier.volume293
dc.identifier.wos000305228200059
dc.language.isoeng
dc.publisherSpringer Science and Business Media LLC
dc.relation.ispartofJournal of Radioanalytical and Nuclear Chemistry
dc.rightsCLOSED
dc.titleThe effect of the housing material on the NaI(Tl) detector response function
dc.typeArticle
dspace.entity.typePublication
local.api.response{"authors":[{"fullName":"Gurler, ORHAN","name":"Orhan","surname":"Gurler","rank":1,"pid":null},{"fullName":"Yalcin, S.","name":"S.","surname":"Yalcin","rank":2,"pid":{"id":{"scheme":"orcid","value":"0000-0001-6779-9230"},"provenance":null}},{"fullName":"Ozmutlu, E. N.","name":"E. N.","surname":"Ozmutlu","rank":3,"pid":null},{"fullName":"Tarim, U. Akar","name":"U. Akar","surname":"Tarim","rank":4,"pid":null}],"openAccessColor":null,"publiclyFunded":false,"type":"publication","language":{"code":"eng","label":"English"},"countries":null,"subjects":[{"subject":{"scheme":"FOS","value":"0103 physical sciences"},"provenance":null},{"subject":{"scheme":"FOS","value":"01 natural sciences"},"provenance":null},{"subject":{"scheme":"FOS","value":"0104 chemical sciences"},"provenance":null}],"mainTitle":"The effect of the housing material on the NaI(Tl) detector response function","subTitle":null,"descriptions":["In this study, a Monte Carlo program has been developed to simulate the response function of the NaI(Tl) detector with all features for 60Co and 137Cs and to investigate the effects of detector housing material on response function. The pulse height spectra in a 2″ × 2″ NaI(Tl) detector due to these gamma ray sources have been measured. Comparison of the experimentally obtained and simulated spectra shows that there is good agreement between both spectra. Energy distributions of gamma photons that generate the backscattering peak in the response function were obtained and the contribution of single, double and multiple Compton scattering events to these distributions was investigated."],"publicationDate":"2012-03-10","publisher":"Springer Science and Business Media LLC","embargoEndDate":null,"sources":["Crossref"],"formats":null,"contributors":null,"coverages":null,"bestAccessRight":{"code":"c_14cb","label":"CLOSED","scheme":"http://vocabularies.coar-repositories.org/documentation/access_rights/"},"container":{"name":"Journal of Radioanalytical and Nuclear Chemistry","issnPrinted":"0236-5731","issnOnline":"1588-2780","issnLinking":null,"ep":"429","iss":null,"sp":"425","vol":"293","edition":null,"conferencePlace":null,"conferenceDate":null},"documentationUrls":null,"codeRepositoryUrl":null,"programmingLanguage":null,"contactPeople":null,"contactGroups":null,"tools":null,"size":null,"version":null,"geoLocations":null,"id":"doi_dedup___::538fcb6a7914e0746138e37ee624a3c1","originalIds":["1716","10.1007/s10967-012-1716-z","50|doiboost____|538fcb6a7914e0746138e37ee624a3c1","2085073500","50|od______9458::39bcc889f3fde79ce259d14decd68b58","c2f84dbd-4561-4df2-a66c-501da7d5a7c7"],"pids":[{"scheme":"doi","value":"10.1007/s10967-012-1716-z"}],"dateOfCollection":null,"lastUpdateTimeStamp":null,"indicators":{"citationImpact":{"citationCount":7,"influence":3.4622556e-9,"popularity":9.73791e-10,"impulse":4,"citationClass":"C5","influenceClass":"C4","impulseClass":"C5","popularityClass":"C5"}},"instances":[{"pids":[{"scheme":"doi","value":"10.1007/s10967-012-1716-z"}],"license":"Springer TDM","type":"Article","urls":["https://doi.org/10.1007/s10967-012-1716-z"],"publicationDate":"2012-03-10","refereed":"peerReviewed"},{"alternateIdentifiers":[{"scheme":"doi","value":"10.1007/s10967-012-1716-z"},{"scheme":"mag_id","value":"2085073500"}],"type":"Article","urls":["https://dx.doi.org/10.1007/s10967-012-1716-z"],"refereed":"nonPeerReviewed"},{"alternateIdentifiers":[{"scheme":"doi","value":"10.1007/s10967-012-1716-z"}],"type":"Article","urls":["https://avesis.uludag.edu.tr/publication/details/c2f84dbd-4561-4df2-a66c-501da7d5a7c7/oai"],"publicationDate":"2012-07-01","refereed":"nonPeerReviewed"}],"isGreen":false,"isInDiamondJournal":false}
local.import.sourceOpenAire
local.indexed.atWOS
local.indexed.atScopus

Dosyalar

Koleksiyonlar

Publications