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dc.contributor.authorBadawi, Ali
dc.contributor.authorPyshkina, Mariia
dc.contributor.authorSusoy, Gulfem
dc.contributor.authorElazaka, Ahmed
dc.contributor.authorEne, Antoaneta
dc.contributor.authorIssa, Shams A. M.
dc.contributor.authorZakaly, Hesham M. H.
dc.contributor.authorTekin, Huseyin O.
dc.contributor.authorSaudi, Heba A.
dc.date.accessioned2021-12-10T10:20:54Z
dc.date.available2021-12-10T10:20:54Z
dc.date.issued2021
dc.identifier.citationIssa S. A. M. , Zakaly H. M. H. , Tekin H. O. , Saudi H. A. , Badawi A., Pyshkina M., Susoy G., Elazaka A., Ene A., "Exploring the FTIR, Optical and Nuclear Radiation Shielding Properties of Samarium-Borate Glass: A Characterization through Experimental and Simulation Methods", NANOMATERIALS, cilt.11, sa.7, 2021
dc.identifier.issn2079-4991
dc.identifier.othervv_1032021
dc.identifier.otherav_39f50014-e018-4fa3-82cd-6cfc0eee0db9
dc.identifier.urihttp://hdl.handle.net/20.500.12627/169711
dc.identifier.urihttps://doi.org/10.3390/nano11071713
dc.description.abstract(Tl2O3)(30)-(Li2O)(10)-(B2O3)((60-y)())-(Sm2O3)(y) glass system with various Sm2O3 additives (y = 0, 0.2, 0.4, 0.6) was studied in detail. The vibrational modes of the (Tl2O3)(30)-(Li2O)(10)-(B2O3)((60-y)) network were active at three composition-related IR spectral peaks that differed from those mixed with Samarium (III) oxide at high wavenumber ranges. These glass samples show that their permeability increased with the Samarium (III) oxide content increase. Additionally, the electronic transition between localized states was observed in the samples. The MAC, HVL, and Zeff values for radiation shielding parameters were calculated in the energy range of 0.015-15 MeV using the FLUKA algorithm. In addition, EBF, EABF, and sigma(R) values were also determined for the prepared glasses. These values indicated that the parameters for shielding (MAC, HVL, Z(eff), EBF, EABF, and sigma(R)) are dependent upon the Samarium (III) oxide content. Furthermore, the addition of Samarium (III) oxide to the examined glass samples greatly reinforced their shielding capacity against gamma photon. The findings of the current study were compared to analyses of the XCOM software, some concretes, and lead. In the experiment, it was found that the SMG0.6 glass sample was the strongest shield.
dc.language.isoeng
dc.subjectStatistical and Nonlinear Physics
dc.subjectKİMYA, MULTİDİSİPLİNER
dc.subjectKimya
dc.subjectTemel Bilimler (SCI)
dc.subjectNANOBİLİM VE NANOTEKNOLOJİ
dc.subjectFizik
dc.subjectMALZEME BİLİMİ, MULTIDISCIPLINARY
dc.subjectMalzeme Bilimi
dc.subjectMühendislik, Bilişim ve Teknoloji (ENG)
dc.subjectFİZİK, UYGULAMALI
dc.subjectYoğun Madde 1:Yapısal, Mekanik ve Termal Özellikler
dc.subjectYüzeyler ve arayüzeyler; İnce filmler ve nanosistemler
dc.subjectBiyokimya
dc.subjectAlkoloidler
dc.subjectTemel Bilimler
dc.subjectMühendislik ve Teknoloji
dc.subjectMetals and Alloys
dc.subjectMaterials Chemistry
dc.subjectChemistry (miscellaneous)
dc.subjectGeneral Materials Science
dc.subjectGeneral Chemistry
dc.subjectPhysical Sciences
dc.titleExploring the FTIR, Optical and Nuclear Radiation Shielding Properties of Samarium-Borate Glass: A Characterization through Experimental and Simulation Methods
dc.typeMakale
dc.relation.journalNANOMATERIALS
dc.contributor.departmentAl-Azhar University Of Gaza , ,
dc.identifier.volume11
dc.identifier.issue7
dc.contributor.firstauthorID2697230


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