New materials of B2O3–Bi2O3–Me2O3 (Me = Yb, Lu) systems
It is shown that the Yb2O3–Bi2O3–B2O3 system gives a new Yb3Bi2B5O15 compound of a hexagonal crystallographic system. Based on the data on the nature of specimens and by means of X-ray study of obtained samples, we determined the boundaries of glass-formation regions in the Yb2O3–Bi2O3–B2O3 syste...
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D.Ghitu Institute of Electronic Engineering and Nanotechnologies
2010
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oai:doaj.org-article:227c97c9e5544255b80486574c17bf702021-11-21T12:03:18ZNew materials of B2O3–Bi2O3–Me2O3 (Me = Yb, Lu) systems2537-63651810-648Xhttps://doaj.org/article/227c97c9e5544255b80486574c17bf702010-12-01T00:00:00Zhttps://mjps.nanotech.md/archive/2010/article/4269https://doaj.org/toc/1810-648Xhttps://doaj.org/toc/2537-6365It is shown that the Yb2O3–Bi2O3–B2O3 system gives a new Yb3Bi2B5O15 compound of a hexagonal crystallographic system. Based on the data on the nature of specimens and by means of X-ray study of obtained samples, we determined the boundaries of glass-formation regions in the Yb2O3–Bi2O3–B2O3 system. Homogeneous glasses were obtained in the following cuts: Bi2O3⋅B2O3 − Lu2O3–B2O3 up to 15 mol % Lu2O3; Lu2O3⋅B2O3−Bi2O3 up to 10 mol % Lu2O3; Bi2O3⋅B2O3 − Lu2O3⋅Bi2O3 up to 15 mol % Lu2O3. Eutectic coordinates of LnBO3– B2O3 (Ln = Се, Pr, Pm, Sm, Tb, Er) systems were calculated at first. Asadov, M.Ahmedova, N.D.Ghitu Institute of Electronic Engineering and NanotechnologiesarticlePhysicsQC1-999ElectronicsTK7800-8360ENMoldavian Journal of the Physical Sciences, Vol 9, Iss 3-4, Pp 280-285 (2010) |
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Physics QC1-999 Electronics TK7800-8360 |
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Physics QC1-999 Electronics TK7800-8360 Asadov, M. Ahmedova, N. New materials of B2O3–Bi2O3–Me2O3 (Me = Yb, Lu) systems |
description |
It is shown that the Yb2O3–Bi2O3–B2O3 system gives a new Yb3Bi2B5O15 compound of
a hexagonal crystallographic system. Based on the data on the nature of specimens and by
means of X-ray study of obtained samples, we determined the boundaries of glass-formation
regions in the Yb2O3–Bi2O3–B2O3 system. Homogeneous glasses were obtained in the following cuts: Bi2O3⋅B2O3 − Lu2O3–B2O3 up to 15 mol % Lu2O3; Lu2O3⋅B2O3−Bi2O3 up to 10 mol
% Lu2O3; Bi2O3⋅B2O3 − Lu2O3⋅Bi2O3 up to 15 mol % Lu2O3. Eutectic coordinates of LnBO3–
B2O3 (Ln = Се, Pr, Pm, Sm, Tb, Er) systems were calculated at first.
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format |
article |
author |
Asadov, M. Ahmedova, N. |
author_facet |
Asadov, M. Ahmedova, N. |
author_sort |
Asadov, M. |
title |
New materials of B2O3–Bi2O3–Me2O3 (Me = Yb, Lu) systems |
title_short |
New materials of B2O3–Bi2O3–Me2O3 (Me = Yb, Lu) systems |
title_full |
New materials of B2O3–Bi2O3–Me2O3 (Me = Yb, Lu) systems |
title_fullStr |
New materials of B2O3–Bi2O3–Me2O3 (Me = Yb, Lu) systems |
title_full_unstemmed |
New materials of B2O3–Bi2O3–Me2O3 (Me = Yb, Lu) systems |
title_sort |
new materials of b2o3–bi2o3–me2o3 (me = yb, lu) systems |
publisher |
D.Ghitu Institute of Electronic Engineering and Nanotechnologies |
publishDate |
2010 |
url |
https://doaj.org/article/227c97c9e5544255b80486574c17bf70 |
work_keys_str_mv |
AT asadovm newmaterialsofb2o3bi2o3me2o3meyblusystems AT ahmedovan newmaterialsofb2o3bi2o3me2o3meyblusystems |
_version_ |
1718419290091159552 |