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dc.contributor.authorTekin, H. O.en
dc.contributor.authorAlmisned, G.en
dc.contributor.authorZakaly, H. M. H.en
dc.contributor.authorZamil, A.en
dc.contributor.authorKhoucheich, D.en
dc.contributor.authorBilal, G.en
dc.contributor.authorAl-Sammarraie, L.en
dc.contributor.authorIssa, S. A. M.en
dc.contributor.authorAl-Buriahi, M. S.en
dc.contributor.authorEne, A.en
dc.date.accessioned2022-05-12T08:31:20Z-
dc.date.available2022-05-12T08:31:20Z-
dc.date.issued2022-
dc.identifier.citationGamma, Neutron, and Heavy Charged Ion Shielding Properties of Er3+-Doped and Sm3+-Doped Zinc Borate Glasses / H. O. Tekin, G. Almisned, H. M. H. Zakaly et al. // Open Chemistry. — 2022. — Vol. 20. — Iss. 1. — P. 130-145.en
dc.identifier.issn2391-5420-
dc.identifier.otherAll Open Access, Gold3
dc.identifier.urihttp://elar.urfu.ru/handle/10995/112256-
dc.description.abstractThis study aimed to investigate the nuclear radiation shielding properties of erbium (Er)-reinforced and samarium (Sm)-reinforced borate glasses. In the 0.015-15 MeV photon energy range, attenuation coefficients, as well as half-value layer tenth-value layers, and the mean-free path have been calculated. Additionally, effective, and equivalent atomic numbers, effective atomic weight, electron density, and exposure and energy absorption build-up factors were also calculated. To evaluate the overall nuclear radiation attenuation competencies of Er-rich and Sm-rich glasses, effective removal cross-section values for fast neutrons and projected range/mass stopping power values for alpha and proton particles were also determined. The glass sample BZBEr2.0 had the highest linear and mass attenuation coefficients (μ and μm), effective conductivity (Ceff), the effective number of electrons (Neff), and effective atomic number (Zeff) values as well as the lowest half-value layer (T1/2), tenth value layers (T1/10), mean free path (λ), exposure build-up factor, and energy absorption build-up factor values. μm values were reported as 2.337, 2.556, 2.770, 2.976, 2.108, 2.266, 2.421, 2.569, and 2.714 for BZBEr0.5, BZBEr1.0, BZBEr1.5, BZBEr2.0, BZBSm0.0, BZBSm0.5, BZBSm1.0, BZBSm1.5, and BZBSm2.0 glass samples at 0.06 MeV, respectively. The results showed that Er has a greater effect than Sm regarding the gamma-ray shielding properties of borate glasses. The results of this investigation could be used in further investigations and added to older investigations with the same aim, to aid the scientific community in determining the most appropriate rare-earth additive, to provide adequate shielding properties based on the requirement. © 2022 Huseyin Ozan Tekin et al., published by De Gruyter.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherDe Gruyter Open Ltden1
dc.publisherWalter de Gruyter GmbHen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceOpen Chem.2
dc.sourceOpen Chemistryen
dc.subjectBORATE GLASSESen
dc.subjectERBIUMen
dc.subjectGAMMA SHIELDINGen
dc.subjectGLASS SHIELDSen
dc.subjectSAMARIUMen
dc.titleGamma, Neutron, and Heavy Charged Ion Shielding Properties of Er3+-Doped and Sm3+-Doped Zinc Borate Glassesen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1515/chem-2022-0128-
dc.identifier.scopus85126324112-
local.contributor.employeeTekin, H.O., Department of Medical Diagnostic Imaging, College of Health Sciences, University of Sharjah, Sharjah, 27272, United Arab Emirates, Computer Engineering Department, Istinye University, Faculty of Engineering and Natural Sciences, Istanbul, 34396, Turkey; Almisned, G., Department of Physics, College of Science, Princess Nourah Bint Abdulrahman University, Riyadh, Saudi Arabia; Zakaly, H.M.H., Institute of Physics and Technology, Ural Federal University, Ekaterinburg, 620002, Russian Federation, Physics Department, Faculty of Science, Al-Azhar University, Assiut, 71452, Egypt; Zamil, A., Department of Medical Diagnostic Imaging, College of Health Sciences, University of Sharjah, Sharjah, 27272, United Arab Emirates; Khoucheich, D., Department of Medical Diagnostic Imaging, College of Health Sciences, University of Sharjah, Sharjah, 27272, United Arab Emirates; Bilal, G., Department of Medical Diagnostic Imaging, College of Health Sciences, University of Sharjah, Sharjah, 27272, United Arab Emirates; Al-Sammarraie, L., Department of Medical Diagnostic Imaging, College of Health Sciences, University of Sharjah, Sharjah, 27272, United Arab Emirates; Issa, S.A.M., Physics Department, Faculty of Science, Al-Azhar University, Assiut, 71452, Egypt, Department of Physics, Faculty of Science, University of Tabuk, Tabuk, Saudi Arabia; Al-Buriahi, M.S., Department of Physics, Sakarya University, Sakarya, Turkey; Ene, A., Department of Chemistry, Physics, and Environment, Dunarea de Jos University of Galati, INPOLDE Research Center, Faculty of Sciences and Environment, 47 Domneasca Street, Galati, 800008, Romaniaen
local.description.firstpage130-
local.description.lastpage145-
local.issue1-
local.volume20-
dc.identifier.wos000764564900001-
local.contributor.departmentDepartment of Medical Diagnostic Imaging, College of Health Sciences, University of Sharjah, Sharjah, 27272, United Arab Emirates; Computer Engineering Department, Istinye University, Faculty of Engineering and Natural Sciences, Istanbul, 34396, Turkey; Department of Physics, College of Science, Princess Nourah Bint Abdulrahman University, Riyadh, Saudi Arabia; Institute of Physics and Technology, Ural Federal University, Ekaterinburg, 620002, Russian Federation; Physics Department, Faculty of Science, Al-Azhar University, Assiut, 71452, Egypt; Department of Physics, Faculty of Science, University of Tabuk, Tabuk, Saudi Arabia; Department of Physics, Sakarya University, Sakarya, Turkey; Department of Chemistry, Physics, and Environment, Dunarea de Jos University of Galati, INPOLDE Research Center, Faculty of Sciences and Environment, 47 Domneasca Street, Galati, 800008, Romaniaen
local.identifier.pure29830060-
local.identifier.eid2-s2.0-85126324112-
local.identifier.wosWOS:000764564900001-
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