4.7 Article

Eu3+-Activated Borogermanate Scintillating Glass with a High Gd2O3 Content

期刊

JOURNAL OF THE AMERICAN CERAMIC SOCIETY
卷 96, 期 5, 页码 1483-1489

出版社

WILEY
DOI: 10.1111/jace.12205

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资金

  1. National Natural Science Fund of China [11165010]
  2. Natural Science Foundation of Jiangxi Province [20114BAB202002]
  3. Department of Education in Jiangxi Province [GJJ12462]
  4. Key Subject of Atomic & Molecular Physics in Jiangxi Province [2011-2015]
  5. Shanghai Key Laboratory of Special Artificial Microstructure Materials and Technology [ammt2012A-8]
  6. Key Laboratory of Transparent Opto-functional Inorganic Materials, Shanghai Institute of Ceramics of Chinese Academy of Sciences
  7. Program for Young Excellent Doctors in Jinggangshan University [JZB007]

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Eu3+-activated borogermanate scintillating glasses with compositions of 25B2O340GeO225Gd2O3(10x)La2O3xEu2O3 were prepared by melt-quenching method. Their optical properties were studied by transmittance, photoluminescence, Fourier transform infrared (FTIR), Raman and X-ray excited luminescence (XEL) spectra in detail. The results suggest that the role of Gd2O3 is of significance for designing dense glass. Furthermore, energy-transfer efficiency from Gd3+ to Eu3+ ions can be near 100% when the content of Eu2O3 exceeds x=4, the corresponding critical distance for Gd3+Eu3+ ion pairs is estimated to be 4.57 angstrom. The strongest emission intensities of Eu3+ ions under both 276 and 394nm excitation are simultaneously at the content of 8mol% Eu2O3. The degree of EuO covalency and the local environment of Eu3+ ions are evaluated by the value of t parameters from JuddOfelt analysis. The calculated results imply that the covalency of EuO bond increases with the increasing concentration of Eu3+ ions in the investigated borogermanate glass. As a potential scintillating application, the strongest XEL intensity under X-ray excitation is found to be in the case of 6mol% Eu2O3, which is slightly different from the photoluminescence results. The possible reason may be attributed to the discrepancy of the excitation mechanism between the ultraviolet and X-ray energy.

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