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dc.contributor.authorTekin, H. O.en
dc.contributor.authorAlmisned, G.en
dc.contributor.authorIssa, S. A. M.en
dc.contributor.authorZakaly, H. M. H.en
dc.contributor.authorKilic, G.en
dc.contributor.authorEne, A.en
dc.date.accessioned2022-10-19T05:20:51Z-
dc.date.available2022-10-19T05:20:51Z-
dc.date.issued2022-
dc.identifier.citationCalculation of NaI(Tl) detector efficiency using 226Ra, 232Th, and 40K radioisotopes: Three-phase Monte Carlo simulation study / H. O. Tekin, G. Almisned, S. A. M. Issa et al. // Open Chemistry. — 2022. — Vol. 20. — Iss. 1. — P. 541-549.en
dc.identifier.issn23915420-
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85133564061&doi=10.1515%2fchem-2022-0169&partnerID=40&md5=aa9a24c9c857367ccb05e5229c53698blink
dc.identifier.urihttp://elar.urfu.ru/handle/10995/117966-
dc.description.abstractThallium-activated sodium iodide (NaI(Tl)) detectors can be used in gamma cameras, environmental radiation assessments, including radiation emission levels from nuclear reactors, and radiation analysis equipment. This three-phase investigation aimed to model a standard NaI(Tl) detector using the Monte Carlo N-Particle eXtended (MCNPX) general-purpose Monte Carlo simulation techniques. Accordingly, a standard NaI(Tl) detector was designed along with the required properties. Next a validation study of the modelled NaI(Tl) detector has been performed based on the experimental results for absolute detector efficiency values obtained from 226Ra, 232Th, and 40K radioisotopes. Our findings indicate that the obtained absolute detector efficiency values are quite close to used experimental values. Finally, we used the modelled detector for determination of mass attenuation coefficients of Ordinary concrete, Lead, Hematite-serpentine concrete, and Steel-scrap concrete at 186.1, 295.22, 351.93, 609.31, 1120.29, 1764.49, 238.63, 911.2, 2614, and 1460.83 keV gamma-ray energies. Additionally, according to our findings, mass attenuation coefficients obtained from the newly designed detector are compatible with the standard NIST (XCOM) data. To conclude, continuous optimisation procedures are strongly suggested for sophisticated Monte Carlo simulations in order to maintain a high degree of simulation reliability. As a result, it can be concluded that the validation of the simulation model is necessary using measured data. Finally, it can also be concluded that the validated detector models are effective instruments for obtaining basic gamma-ray shielding parameters such as mass attenuation coefficients. © 2022 Huseyin Ozan Tekin et al., published by De Gruyter.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherDe Gruyter Open Ltden
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceOpen Chemistryen
dc.subjectABSOLUTE DETECTOR EFFICIENCYen
dc.subjectMCNPXen
dc.subjectNAI(TL) DETECTORen
dc.subjectSCINTILLATION DETECTORSen
dc.titleCalculation of NaI(Tl) detector efficiency using 226Ra, 232Th, and 40K radioisotopes: Three-phase Monte Carlo simulation studyen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1515/chem-2022-0169-
dc.identifier.scopus85133564061-
local.contributor.employeeTekin, H.O., Medical Diagnostic Imaging Department, College of Health Sciences, University of Sharjah, Sharjah, 27272, United Arab Emirates, Computer Engineering Department, Faculty of Engineering and Natural Sciences, Istinye University, Istanbul, 34396, Turkeyen
local.contributor.employeeAlmisned, G., Department of Physics, College of Science, Princess Nourah Bint Abdulrahman University, P.O. Box 84428, Riyadh, 11671, Saudi Arabiaen
local.contributor.employeeIssa, S.A.M., Physics Department, Faculty of Science, University of Tabuk, Tabuk, 71451, Saudi Arabia, Physics Department, Faculty of Science, Al-Azhar University, Assiut, 71524, Egypten
local.contributor.employeeZakaly, H.M.H., Physics Department, Faculty of Science, Al-Azhar University, Assiut, 71524, Egypt, Institute of Physics and Technology, Ural Federal University, Ekaterinburg, 620002, Russian Federationen
local.contributor.employeeKilic, G., Department of Physics, Faculty of Science and Letters, Eskisehir Osmangazi University, Eskisehir, TR-26040, Turkeyen
local.contributor.employeeEne, A., Department of Physics, Faculty of Science and Letters, Eskisehir Osmangazi University, Eskisehir, TR-26040, Turkeyen
local.description.firstpage541-
local.description.lastpage549-
local.issue1-
local.volume20-
dc.identifier.wos000817962500001-
local.contributor.departmentMedical Diagnostic Imaging Department, College of Health Sciences, University of Sharjah, Sharjah, 27272, United Arab Emiratesen
local.contributor.departmentComputer Engineering Department, Faculty of Engineering and Natural Sciences, Istinye University, Istanbul, 34396, Turkeyen
local.contributor.departmentDepartment of Physics, College of Science, Princess Nourah Bint Abdulrahman University, P.O. Box 84428, Riyadh, 11671, Saudi Arabiaen
local.contributor.departmentPhysics Department, Faculty of Science, University of Tabuk, Tabuk, 71451, Saudi Arabiaen
local.contributor.departmentPhysics Department, Faculty of Science, Al-Azhar University, Assiut, 71524, Egypten
local.contributor.departmentInstitute of Physics and Technology, Ural Federal University, Ekaterinburg, 620002, Russian Federationen
local.contributor.departmentDepartment of Physics, Faculty of Science and Letters, Eskisehir Osmangazi University, Eskisehir, TR-26040, Turkeyen
local.identifier.pure30621465-
local.identifier.eid2-s2.0-85133564061-
local.identifier.wosWOS:000817962500001-
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