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Structure and Physical Properties of the Barium Niobium Sulfides BaNbS 3 and BaNb 0.8S 3-δ
BaNb 0.8S 3-δ and BaNbS 3 were prepared by heating desired amounts of BaCO 3 and Nb 2O 5 under CS 2/N 2 flow. We found that nominal composition of BaNb 0.8S has sulfur defect, and therefore should be written as BaNb 0.8S 3-δ. XANES experiments of Nb K-edges and XPS experiments proved that the oxidat...
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Published in: | Journal of solid state chemistry 1995, Vol.115 (2), p.427-434 |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Online Access: | Get full text |
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Summary: | BaNb
0.8S
3-δ and BaNbS
3 were prepared by heating desired amounts of BaCO
3 and Nb
2O
5 under CS
2/N
2 flow. We found that nominal composition of BaNb
0.8S has sulfur defect, and therefore should be written as BaNb
0.8S
3-δ. XANES experiments of Nb
K-edges and XPS experiments proved that the oxidation state of Nb is the same in BaNb
0.8S
3-δ and BaNbS
3. To understand their structures, the electronic and physical properties of the Ba
MX
3 (
M = V, Nb,
X = S;
M = Ta,
X = S, Se) phases are compared. In spite of their structural similarity, they exhibit rather different physical properties. It has been known that BaVS
3 is a metal and undergoes a metal to semiconductor transition at 130 K, and this phase shows the ferro antiferromagnetic transition at a lower temperature. However, BaNbS
3 and BaTaS
3 are diamagnetic semiconductors at room temperature. The major factor stabilizing the semiconducting state for BaTa
X
3 and BaNbS
3 may be a large spin-orbit coupling rather than a structural distortion. |
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ISSN: | 0022-4596 1095-726X |
DOI: | 10.1006/jssc.1995.1155 |