<p>This work examined the physical, dielectric, and gamma-ray shielding properties of the (65-<i>x</i>) P<sub>2</sub>O<sub>5</sub>-15 Li<sub>2</sub>O-15ZnO-5Bi<sub>2</sub>O<sub>3</sub>-<i>x</i>Sb<sub>2</sub>O<sub>3</sub> glass system in relation to Sb<sub>2</sub>O<sub>3</sub>. The density of glass specimens rises rapidly as Sb<sub>2</sub>O<sub>3</sub> replaces P<sub>2</sub>O<sub>5</sub>. A little shift in the FTIR principal bands is observed upon the addition of Sb<sub>2</sub>O<sub>3</sub>, and this shift is directly linked to the phosphate network depolymerizing, which changes the P-O-P bond length. In the frequency spanning from 50 to 5&#xa0;MHz, the dielectric spectroscopy of specimens of glass was examined as a function of frequency. Up to 2.0&#xa0;mol%, the dielectric constant falls as Sb<sub>2</sub>O<sub>3</sub> concentration rises and increases beyond that point. The XCOM and the Phy-X/PSD software were utilized to determine the glass mean free path, which included the energy range of 0.01-10&#xa0;MeV. Similar outcomes were obtained with both methods. Furthermore, mean free path, buildup factors, and transmission factors were computed to determine the glass samples’ shielding efficiency. As the Sb<sub>2</sub>O<sub>3</sub> concentration in mol.% rose, the radiation shielding properties in the samples under investigation showed a significant improvement, with an order of Sb-4.0 &gt; Sb-3.0 &gt; Sb-2.0 &gt; Sb-1.0 &gt; Sb-0.0 observed at all photon energies. These results demonstrate how very promising the examined glasses are as materials for radiation shielding. Addition of Sb<sub>2</sub>O<sub>3</sub> to the zinc bismuth phosphate glass system alters all optical parameters, including the real part, <i>ε</i>1, and imaginary part, <i>ε</i><sub>2</sub>, of the dielectric constant, extinction coefficient (<i>k</i>), and refractive index (<i>n</i>). There is strong transmittance throughout the visible light band and high reflection within the ultraviolet, as indicated by the transmittance (<i>T</i>) as well as reflectance (<i>R</i>) fluctuating with wavelength (<i>λ</i>).</p>

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Antimony-Doped Phosphate Glasses: Production, Structure, Optical, Dielectric Features, and Gamma Attenuation Attributes

  • Gharam A. Alharshan,
  • Nasra M. Ebrahem,
  • Shaaban M. Shaaban,
  • Shimaa Ali Said,
  • R. A. Elsad,
  • Yehya I. Mesalam,
  • A. M. A. Mahmoud

摘要

This work examined the physical, dielectric, and gamma-ray shielding properties of the (65-x) P2O5-15 Li2O-15ZnO-5Bi2O3-xSb2O3 glass system in relation to Sb2O3. The density of glass specimens rises rapidly as Sb2O3 replaces P2O5. A little shift in the FTIR principal bands is observed upon the addition of Sb2O3, and this shift is directly linked to the phosphate network depolymerizing, which changes the P-O-P bond length. In the frequency spanning from 50 to 5 MHz, the dielectric spectroscopy of specimens of glass was examined as a function of frequency. Up to 2.0 mol%, the dielectric constant falls as Sb2O3 concentration rises and increases beyond that point. The XCOM and the Phy-X/PSD software were utilized to determine the glass mean free path, which included the energy range of 0.01-10 MeV. Similar outcomes were obtained with both methods. Furthermore, mean free path, buildup factors, and transmission factors were computed to determine the glass samples’ shielding efficiency. As the Sb2O3 concentration in mol.% rose, the radiation shielding properties in the samples under investigation showed a significant improvement, with an order of Sb-4.0 > Sb-3.0 > Sb-2.0 > Sb-1.0 > Sb-0.0 observed at all photon energies. These results demonstrate how very promising the examined glasses are as materials for radiation shielding. Addition of Sb2O3 to the zinc bismuth phosphate glass system alters all optical parameters, including the real part, ε1, and imaginary part, ε2, of the dielectric constant, extinction coefficient (k), and refractive index (n). There is strong transmittance throughout the visible light band and high reflection within the ultraviolet, as indicated by the transmittance (T) as well as reflectance (R) fluctuating with wavelength (λ).