Impact of B2O3 on Physical, Optical Characteristics and Radiation Attenuation Factors of Borotellurite Glasses | Research Square window.SnipcartSettings = { analytics: { enabled: false } }; (function() { var accessVector = localStorage.getItem('access_vector') || ''; window.dataLayer = window.dataLayer || []; if (accessVector) { window.dataLayer.push({ user: { profile: { profileInfo: { snid: accessVector } } } }); } })(); (function(w,d,s,l,i){w[l]=w[l]||[];w[l].push({'gtm.start':new Date().getTime(),event:'gtm.js'});var f=d.getElementsByTagName(s)[0],j=d.createElement(s),dl=l!='dataLayer'?'&l='+l:'';j.async=true;j.src='https://www.googletagmanager.com/gtm.js?id='+i+dl;f.parentNode.insertBefore(j,f);})(window,document,'script','dataLayer','GTM-K279D39R'); Browse Preprints In Review Journals COVID-19 Preprints AJE Video Bytes Research Tools Research Promotion AJE Professional Editing AJE Rubriq About Preprint Platform In Review Editorial Policies Our Team Advisory Board Help Center Sign In Submit a Preprint Cite Share Download PDF Research Article Impact of B2O3 on Physical, Optical Characteristics and Radiation Attenuation Factors of Borotellurite Glasses R. El-Mallawany, Weam aboutaleb, M.A. Naeem, S.M. Kotb, M.E. Krar, and 1 more This is a preprint; it has not been peer reviewed by a journal. https://doi.org/ 10.21203/rs.3.rs-1231390/v1 This work is licensed under a CC BY 4.0 License Status: Published Journal Publication published 28 Feb, 2022 Read the published version in Journal of Materials Research and Technology → Version 1 posted You are reading this latest preprint version Abstract Borotellurite glasses with a composition [(60-X)TeO 2 -(20+X)B 2 O 3 -10Li 2 O-10Bi 2 O 3 ] where x= 5-20 in steps of 5 mol% have been synthesized. Glass density, molar volume, oxygen packing density, and many other physical parameters were measured. UV-spectra in the wave length range (200-800) nm have been measured for the whole glass series. The optical energy band gap E opt , refractive index, and optical basicity were measured. The mass absorption coefficients (μ m ) are determined experimentally by the HPGe detector and compared with the theoretical values obtained by XCOM program and MCNP5 simulation code within (0.121–1.408) MeV photon energy range. Half value layer (HVL), effective atomic number and electron density (Z eff and N eff ), and macroscopic removal cross-section (∑R) were evaluated. The sample [55TeO 2 – 25B 2 O 3 – 10Bi 2 O 3 – 10Li 2 O] possess the highest values of (μ m = 1.192 ± 0.033 cm 2 /g, Z eff = 56.12 e/atom and ∑ R = 0.101499 cm -1 ) at energy 121 keV also lower values of (HVL = 0.121 cm, TVL = 0.1 cm and MFP = 0.174 cm) at photon energy 121 keV, therefore this sample considered the best gamma ray shielding material among the prepared glasses. Inorganic Chemistry Organic Chemistry Glasses Optical properties Radiation shielding MCNP5 code XCOM software Full Text Cite Share Download PDF Status: Published Journal Publication published 28 Feb, 2022 Read the published version in Journal of Materials Research and Technology → Version 1 posted You are reading this latest preprint version Research Square lets you share your work early, gain feedback from the community, and start making changes to your manuscript prior to peer review in a journal. As a division of Research Square Company, we’re committed to making research communication faster, fairer, and more useful. We do this by developing innovative software and high quality services for the global research community. Our growing team is made up of researchers and industry professionals working together to solve the most critical problems facing scientific publishing. Also discoverable on Platform About Our Team In Review Editorial Policies Advisory Board Help Center Resources Author Services Accessibility API Access RSS feed Manage Cookie Preferences © Research Square 2026 | ISSN 2693-5015 (online) Privacy Policy Terms of Service Do Not Sell My Personal Information {"props":{"pageProps":{"initialData":{"identity":"rs-1231390","acceptedTermsAndConditions":true,"allowDirectSubmit":true,"archivedVersions":[],"articleType":"Research Article","associatedPublications":[],"authors":[{"id":74626227,"identity":"50b801e6-8437-401a-a431-0ae7dbd4d9a8","order_by":0,"name":"R. 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[email protected]","identity":"researchsquare","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":true,"externalIdentity":"","sideBox":"","snPcode":"","submissionUrl":"/submission","title":"Research Square","twitterHandle":"researchsquare","acdcEnabled":true,"dfaEnabled":false,"editorialSystem":"","reportingPortfolio":"","inReviewEnabled":false,"inReviewRevisionsEnabled":true},"keywords":"Glasses, Optical properties, Radiation shielding, MCNP5 code, XCOM software","lastPublishedDoi":"10.21203/rs.3.rs-1231390/v1","lastPublishedDoiUrl":"https://doi.org/10.21203/rs.3.rs-1231390/v1","license":{"name":"CC BY 4.0","url":"https://creativecommons.org/licenses/by/4.0/"},"manuscriptAbstract":"\u003cp\u003eBorotellurite glasses with a composition [(60-X)TeO\u003csub\u003e2\u003c/sub\u003e-(20+X)B\u003csub\u003e2\u003c/sub\u003eO\u003csub\u003e3\u003c/sub\u003e-10Li\u003csub\u003e2\u003c/sub\u003eO-10Bi\u003csub\u003e2\u003c/sub\u003eO\u003csub\u003e3\u003c/sub\u003e] where x= 5-20 in steps of 5 mol% have been synthesized.\u0026nbsp;Glass density, molar volume, oxygen packing density, and many other physical parameters were measured. UV-spectra in the wave length range (200-800) nm have been measured for the whole glass series. The optical energy band gap \u003cem\u003eE\u003c/em\u003e\u003csub\u003eopt\u003c/sub\u003e , refractive index, and optical basicity were measured.\u0026nbsp;The mass absorption coefficients (μ\u003csub\u003em\u003c/sub\u003e) are determined experimentally by the HPGe detector and compared with the theoretical values obtained by XCOM program and MCNP5 simulation code within (0.121–1.408) MeV photon energy range. Half value layer (HVL), effective atomic number and electron density (Z\u003csub\u003eeff\u003c/sub\u003e and N\u003csub\u003eeff\u003c/sub\u003e), and macroscopic removal cross-section (∑R) were evaluated. The sample [55TeO\u003csub\u003e2\u003c/sub\u003e – 25B\u003csub\u003e2\u003c/sub\u003eO\u003csub\u003e3\u003c/sub\u003e – 10Bi\u003csub\u003e2\u003c/sub\u003eO\u003csub\u003e3\u003c/sub\u003e – 10Li\u003csub\u003e2\u003c/sub\u003eO] possess the highest values of (μ\u003csub\u003em\u003c/sub\u003e = 1.192 ± 0.033 cm\u003csup\u003e2\u003c/sup\u003e/g, Z\u003csub\u003eeff\u003c/sub\u003e = 56.12 e/atom and ∑ R = 0.101499 cm\u003csup\u003e-1\u003c/sup\u003e) at energy 121 keV also lower values of (HVL = 0.121 cm, TVL = 0.1 cm and MFP = 0.174 cm) at photon energy 121 keV, therefore this sample considered the best gamma ray shielding material among the prepared glasses.\u003c/p\u003e","manuscriptTitle":"Impact of B2O3 on Physical, Optical Characteristics and Radiation Attenuation Factors of Borotellurite Glasses","msid":"","msnumber":"","nonDraftVersions":[{"code":1,"date":"2022-01-07 14:33:34","doi":"10.21203/rs.3.rs-1231390/v1","editorialEvents":[{"type":"communityComments","content":0}],"status":"published","journal":{"display":true,"email":"
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