Maryam Al Huwayz, A. M. Abdelghany, R. A. Elsad, Shaaban M. Shaaban, Y. S. Rammah, S. M. Kotb, S. Talaat, A. S. Abouhaswa
{"title":"掺杂不同浓度氧化镉的硼碲玻璃的制造、结构、光学和伽马射线衰减特性","authors":"Maryam Al Huwayz, A. M. Abdelghany, R. A. Elsad, Shaaban M. Shaaban, Y. S. Rammah, S. M. Kotb, S. Talaat, A. S. Abouhaswa","doi":"10.1007/s11082-024-07120-0","DOIUrl":null,"url":null,"abstract":"<div><p>Glass samples of CdO doped bario-fluoride borotellurite with nominal compositions of (45-x)B<sub>2</sub>O<sub>3</sub> + 30TeO<sub>2</sub> + 15BaF<sub>2</sub> + 10Li<sub>2</sub>O + xCdO and substitution ratios of x = 0.0 (Cd0.0), 0.5 (Cd0.5), 2.0 (Cd2.0), 4.0 (Cd4.0), and 7.0 (Cd7.0) mol% were synthesized using the well-known melt quenching process. The structure, physical, and optical characteristics of the prepared glasses have been investigated. The Phy-X/PSD software employed to evaluate the radiation attenuation competence of the prepared glasses. The XRD analysis confirmed that the Cd-0.0/Cd-7.0 samples were in amorphous nature. Density (ρ) varied from 3.8633 g/cm<sup>3</sup> for Cd-0.0 sample to 4.2894 g/cm<sup>3</sup> for Cd-7.0 sample. The molar volume (V<sub>m</sub>) varied from 28.08 cm<sup>3</sup>/mol to 26.25 cm<sup>3</sup>/mol. The inclusion of CdO in the glasses network reduced the direct band gaps from 3.54 eV to 3.196 eV and the indirect band gaps from 3.23 eV to 2.85 eV, respectively. Urbach’s energy changed from 0.23 eV to 0.318 eV and refractive index (n) ranged between 2.333 and 2.439. Mass-absorption coefficient (MAC) values ranged between 30.696 − 0.032 cm<sup>2</sup>/g, 30.825–0.032 cm<sup>2</sup>/g, 31.210–0.032 cm<sup>2</sup>/g, 31.714–0.033 cm<sup>2</sup>/g and 32.450–0.033 cm<sup>2</sup>/g, for Cd0.0, Cd0.5, Cd2.0, Cd4.0, and Cd7.0 glass samples, respectively. Sample coded as Cd7.0 possessed the minimum half value layer (HVL) which ranged from 0.005 cm to 4.887 cm at photon energy 0.015 and 15 MeV, respectively. The effective atomic number (Z<sub>eff</sub>) and effective ion density (N<sub>eff</sub>) possessed the same trend of MAC parameter. Results confirmed that the present glasses are superior as γ-ray shields compared to other commercial materials.</p></div>","PeriodicalId":720,"journal":{"name":"Optical and Quantum Electronics","volume":"56 12","pages":""},"PeriodicalIF":3.3000,"publicationDate":"2024-11-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Fabrication, structure, optical and gamma-ray attenuation properties of borotellurite glasses doped with variable concentrations of cadmium oxide\",\"authors\":\"Maryam Al Huwayz, A. M. Abdelghany, R. A. Elsad, Shaaban M. Shaaban, Y. S. Rammah, S. M. Kotb, S. Talaat, A. S. Abouhaswa\",\"doi\":\"10.1007/s11082-024-07120-0\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Glass samples of CdO doped bario-fluoride borotellurite with nominal compositions of (45-x)B<sub>2</sub>O<sub>3</sub> + 30TeO<sub>2</sub> + 15BaF<sub>2</sub> + 10Li<sub>2</sub>O + xCdO and substitution ratios of x = 0.0 (Cd0.0), 0.5 (Cd0.5), 2.0 (Cd2.0), 4.0 (Cd4.0), and 7.0 (Cd7.0) mol% were synthesized using the well-known melt quenching process. The structure, physical, and optical characteristics of the prepared glasses have been investigated. The Phy-X/PSD software employed to evaluate the radiation attenuation competence of the prepared glasses. The XRD analysis confirmed that the Cd-0.0/Cd-7.0 samples were in amorphous nature. Density (ρ) varied from 3.8633 g/cm<sup>3</sup> for Cd-0.0 sample to 4.2894 g/cm<sup>3</sup> for Cd-7.0 sample. The molar volume (V<sub>m</sub>) varied from 28.08 cm<sup>3</sup>/mol to 26.25 cm<sup>3</sup>/mol. The inclusion of CdO in the glasses network reduced the direct band gaps from 3.54 eV to 3.196 eV and the indirect band gaps from 3.23 eV to 2.85 eV, respectively. Urbach’s energy changed from 0.23 eV to 0.318 eV and refractive index (n) ranged between 2.333 and 2.439. Mass-absorption coefficient (MAC) values ranged between 30.696 − 0.032 cm<sup>2</sup>/g, 30.825–0.032 cm<sup>2</sup>/g, 31.210–0.032 cm<sup>2</sup>/g, 31.714–0.033 cm<sup>2</sup>/g and 32.450–0.033 cm<sup>2</sup>/g, for Cd0.0, Cd0.5, Cd2.0, Cd4.0, and Cd7.0 glass samples, respectively. Sample coded as Cd7.0 possessed the minimum half value layer (HVL) which ranged from 0.005 cm to 4.887 cm at photon energy 0.015 and 15 MeV, respectively. The effective atomic number (Z<sub>eff</sub>) and effective ion density (N<sub>eff</sub>) possessed the same trend of MAC parameter. Results confirmed that the present glasses are superior as γ-ray shields compared to other commercial materials.</p></div>\",\"PeriodicalId\":720,\"journal\":{\"name\":\"Optical and Quantum Electronics\",\"volume\":\"56 12\",\"pages\":\"\"},\"PeriodicalIF\":3.3000,\"publicationDate\":\"2024-11-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Optical and Quantum Electronics\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s11082-024-07120-0\",\"RegionNum\":3,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Optical and Quantum Electronics","FirstCategoryId":"5","ListUrlMain":"https://link.springer.com/article/10.1007/s11082-024-07120-0","RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
Fabrication, structure, optical and gamma-ray attenuation properties of borotellurite glasses doped with variable concentrations of cadmium oxide
Glass samples of CdO doped bario-fluoride borotellurite with nominal compositions of (45-x)B2O3 + 30TeO2 + 15BaF2 + 10Li2O + xCdO and substitution ratios of x = 0.0 (Cd0.0), 0.5 (Cd0.5), 2.0 (Cd2.0), 4.0 (Cd4.0), and 7.0 (Cd7.0) mol% were synthesized using the well-known melt quenching process. The structure, physical, and optical characteristics of the prepared glasses have been investigated. The Phy-X/PSD software employed to evaluate the radiation attenuation competence of the prepared glasses. The XRD analysis confirmed that the Cd-0.0/Cd-7.0 samples were in amorphous nature. Density (ρ) varied from 3.8633 g/cm3 for Cd-0.0 sample to 4.2894 g/cm3 for Cd-7.0 sample. The molar volume (Vm) varied from 28.08 cm3/mol to 26.25 cm3/mol. The inclusion of CdO in the glasses network reduced the direct band gaps from 3.54 eV to 3.196 eV and the indirect band gaps from 3.23 eV to 2.85 eV, respectively. Urbach’s energy changed from 0.23 eV to 0.318 eV and refractive index (n) ranged between 2.333 and 2.439. Mass-absorption coefficient (MAC) values ranged between 30.696 − 0.032 cm2/g, 30.825–0.032 cm2/g, 31.210–0.032 cm2/g, 31.714–0.033 cm2/g and 32.450–0.033 cm2/g, for Cd0.0, Cd0.5, Cd2.0, Cd4.0, and Cd7.0 glass samples, respectively. Sample coded as Cd7.0 possessed the minimum half value layer (HVL) which ranged from 0.005 cm to 4.887 cm at photon energy 0.015 and 15 MeV, respectively. The effective atomic number (Zeff) and effective ion density (Neff) possessed the same trend of MAC parameter. Results confirmed that the present glasses are superior as γ-ray shields compared to other commercial materials.
期刊介绍:
Optical and Quantum Electronics provides an international forum for the publication of original research papers, tutorial reviews and letters in such fields as optical physics, optical engineering and optoelectronics. Special issues are published on topics of current interest.
Optical and Quantum Electronics is published monthly. It is concerned with the technology and physics of optical systems, components and devices, i.e., with topics such as: optical fibres; semiconductor lasers and LEDs; light detection and imaging devices; nanophotonics; photonic integration and optoelectronic integrated circuits; silicon photonics; displays; optical communications from devices to systems; materials for photonics (e.g. semiconductors, glasses, graphene); the physics and simulation of optical devices and systems; nanotechnologies in photonics (including engineered nano-structures such as photonic crystals, sub-wavelength photonic structures, metamaterials, and plasmonics); advanced quantum and optoelectronic applications (e.g. quantum computing, memory and communications, quantum sensing and quantum dots); photonic sensors and bio-sensors; Terahertz phenomena; non-linear optics and ultrafast phenomena; green photonics.