Gamma ray shielding behavior of Li2O-doped PbO–MoO3–B2O3 glass system

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Özet

In this work, five glasses for radiation shielding applications in the composition of (30 + x) PbO–5 MoO3–(25 − x) Li2O–40 B2O3 (where x = 0, 5, 10, 15 and 20 mol%) have been prepared. The density increases from 4.354 to 6.578 g cm−3 and the molar volume decreases from 25.144 to 22.520 cm3 with the replacement of Li2O by PbO. The indirect and direct band gap energies decrease from (2.2870–2.2297) eV and (2.9619–2.8660) eV, respectively, as lead content increases from 30 to 50 mol%. In addition, the refractive index of the samples lies between 2.6214 and 2.6429. Geant4 simulation code has been used to evaluate the gamma photon transmission through the prepared samples. Pb50Li5 sample has lower transmission fraction among the studied glasses. For the 2-cm glass thickness, the transmission fraction of Pb30Li25 sample was found to be 0.433 while at the same thickness the transmission fraction of Pb50Li5 sample is 0.265. At 1173 keV, the HVL values were found to be 1.752 cm for Pb50Li5 and 2.693 cm for Pb30Li25 glasses. At the same photon energy, the MFP values were calculated to be 2.529 cm and 3.886 cm for the Pb50Li5 and Pb30Li25 samples, respectively. Due to the higher Pb content existing in the Pb50Li5 glass, this glass effectively blocks the gamma rays compared to the other samples.

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https://doi.org/10.1007/s00339-019-2964-3Yayıncı resmi DOI adresi
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AlanDeğerDil
dc.contributor.authorAli, Atif Mossad
dc.contributor.authorSayyed, M.I.
dc.contributor.authorRashad, M.
dc.contributor.authorKumar, Ashok
dc.contributor.authorKaur, Ramandeep
dc.contributor.authorAşkın, A.
dc.contributor.authorAlgarni, H.
dc.date.accessioned2026-10-28T14:57:07.924857743Z
dc.date.available2026-10-28T14:57:07.924857743Z
dc.date.issued2019
dc.description.abstractIn this work, five glasses for radiation shielding applications in the composition of (30 + x) PbO–5 MoO3–(25 − x) Li2O–40 B2O3 (where x = 0, 5, 10, 15 and 20 mol%) have been prepared. The density increases from 4.354 to 6.578 g cm−3 and the molar volume decreases from 25.144 to 22.520 cm3 with the replacement of Li2O by PbO. The indirect and direct band gap energies decrease from (2.2870–2.2297) eV and (2.9619–2.8660) eV, respectively, as lead content increases from 30 to 50 mol%. In addition, the refractive index of the samples lies between 2.6214 and 2.6429. Geant4 simulation code has been used to evaluate the gamma photon transmission through the prepared samples. Pb50Li5 sample has lower transmission fraction among the studied glasses. For the 2-cm glass thickness, the transmission fraction of Pb30Li25 sample was found to be 0.433 while at the same thickness the transmission fraction of Pb50Li5 sample is 0.265. At 1173 keV, the HVL values were found to be 1.752 cm for Pb50Li5 and 2.693 cm for Pb30Li25 glasses. At the same photon energy, the MFP values were calculated to be 2.529 cm and 3.886 cm for the Pb50Li5 and Pb30Li25 samples, respectively. Due to the higher Pb content existing in the Pb50Li5 glass, this glass effectively blocks the gamma rays compared to the other samples.
dc.description.sponsorshipDeanship of Scientific Research, King Faisal University, DSR, KFU, (R.G.P. 2/33/40)
dc.description.sponsorshipDeanship of Scientific Research, King Faisal University, DSR, KFU
dc.identifier.articlenumber671
dc.identifier.doi10.1007/s00339-019-2964-3
dc.identifier.eissn1432-0630
dc.identifier.issn0947-8396
dc.identifier.issue10
dc.identifier.scopus2-s2.0-85071744319
dc.identifier.urihttps://rdlopen.rawdatalibrary.net/r/munzur/3793
dc.identifier.volume125
dc.identifier.wosWOS:000485036400001
dc.language.isoen
dc.publisherSpringer Verlag
dc.relation.ispartofApplied Physics A: Materials Science and Processing
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.subject.otherBinary alloys
dc.subject.otherEnergy gap
dc.subject.otherGlass
dc.subject.otherLead oxide
dc.subject.otherMolybdenum oxide
dc.subject.otherPhotons
dc.subject.otherRadiation shielding
dc.subject.otherRefractive index
dc.subject.otherDirect band gap
dc.subject.otherGamma photons
dc.subject.otherGamma-ray shielding
dc.subject.otherGEANT4 simulation
dc.subject.otherGlass systems
dc.subject.otherGlass thickness
dc.subject.otherPhoton energy
dc.subject.otherShielding applications
dc.subject.otherGamma rays
dc.titleGamma ray shielding behavior of Li2O-doped PbO–MoO3–B2O3 glass system
dc.typeArticle
rdl.citation.openalex24
rdl.citation.scopus21
rdl.oa.statusclosed
rdl.scopus.quartileQ2
rdl.source.indexSCOPUS
rdl.source.indexWOS