Luminescence property of rare-earth-doped bismuth-borate glasses with different concentrations of bismuth and rare-earth material

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Author listPark J.M., Kim H.J., Limsuwan P., Kaewkhao J.

Publication year2012

Volume number61

Issue number2

Start page248

End page253

Number of pages6

ISSN0374-4884

eISSN0374-4884

URLhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-84866363457&doi=10.3938%2fjkps.61.248&partnerID=40&md5=477f466b8cf2cbfd54e45776a2d15352

LanguagesEnglish-Great Britain (EN-GB)


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Abstract

Bismuth-borate glass scintillators have high density and good radiation hardness. Thus, if they are highly luminescent, they can be applied in astrophysics, high-energy and nuclear physics, homeland security, radiation detection and medical imaging. Bismuth-borate glasseswith the formula xBi 2O 3:(100 - x)B 2O 3 (x = 30, 50, and 66. 7 mol%) were fabricated and doped with Nd, Er, Dy, Pr, Sm, Ho, Gd, and Ce in different dopant concentrations by using the melt-quenching technique. The X-ray emission spectra for the bismuth-borate glasses were measured and showed that only Sm-, Dy-, and Nd-doped glass scintillators had noticeable luminescence. Also, we measured the photo-luminescence and the proton-induced emission spectra. We obtained the result that Sm- and Dy- doped glass scintillators emitted luminescence. The emission peaks of the Sm- doped glass were 569, 598, 641, and 708 nm and were due to ( 4G 5/2 → 6H J) (J = 5/2, 7/2, 9/2, 11/2) transitions, respectively. The emission peaks of the Dy- doped glass were at 485 nm ( 4F 9/2 → 6H 15/2), 575 nm ( 4F 9/2 → 6H 13/2), 660 nm ( 4F 9/2 → 6H 11/2), and 755 nm ( 4F 9/2 → 6H 9/2 + 6H 11/2), and that of the Nd-doped glass was at 895 nm due to the ( 4F 3/2 → 4I 9/2) transition. The luminescence intensities were compared in terms of different Bi concentrations and dopant concentrations. © 2012 The Korean Physical Society.


Keywords

Bismuth-borate glassRare-earthScintillator


Last updated on 2023-26-09 at 07:35