Structure and orientation of a superconducting Y-Ba-Cu-O thin film on zirconia substrate. A study by micro-Raman spectroscopy
A thin film of YBa 2Cu 3O x deposited on Zirconia (100) substrate, and transiting at 92 K was examined by micro-Raman spectroscopy. The layer is revealed to be an aggregation of two types of micro-crystals: one of them is oriented with the c axis nearly perpendicular to the surface and having often...
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Veröffentlicht in: | Solid state communications 1989-10, Vol.72 (2), p.191-194 |
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container_title | Solid state communications |
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creator | Huong, Pham V. Bruyere, J.C. Bustarret, E. Granchamp, P. |
description | A thin film of YBa
2Cu
3O
x deposited on Zirconia (100) substrate, and transiting at 92 K was examined by micro-Raman spectroscopy. The layer is revealed to be an aggregation of two types of micro-crystals: one of them is oriented with the
c axis nearly perpendicular to the surface and having often truncatures which give them the appearance of nearly square pyramids, and the others with the
c axis parallel to the surface.
The oxygen content is evaluated to be
x = 6.97, therefore the formula of the superconducting material could be YBa
2Cu
3O
7. This oxygen amount is relatively homogeneous at various areas on the surface even where the distribution of the crystal aggregate is not homogeneous. After six months, a lost of oxygen, down to
x = 6.8 in the same sample is recorded.
These micro-crystals appear to grow on a continuous ground which was identified as a green phase, Y
2BaCuO
5 resulting from the interaction at the interface between YBa
2Cu
3O
7 and the substrate dopped itself with Y
2O
3. |
doi_str_mv | 10.1016/0038-1098(89)90521-8 |
format | Article |
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2Cu
3O
x deposited on Zirconia (100) substrate, and transiting at 92 K was examined by micro-Raman spectroscopy. The layer is revealed to be an aggregation of two types of micro-crystals: one of them is oriented with the
c axis nearly perpendicular to the surface and having often truncatures which give them the appearance of nearly square pyramids, and the others with the
c axis parallel to the surface.
The oxygen content is evaluated to be
x = 6.97, therefore the formula of the superconducting material could be YBa
2Cu
3O
7. This oxygen amount is relatively homogeneous at various areas on the surface even where the distribution of the crystal aggregate is not homogeneous. After six months, a lost of oxygen, down to
x = 6.8 in the same sample is recorded.
These micro-crystals appear to grow on a continuous ground which was identified as a green phase, Y
2BaCuO
5 resulting from the interaction at the interface between YBa
2Cu
3O
7 and the substrate dopped itself with Y
2O
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2Cu
3O
x deposited on Zirconia (100) substrate, and transiting at 92 K was examined by micro-Raman spectroscopy. The layer is revealed to be an aggregation of two types of micro-crystals: one of them is oriented with the
c axis nearly perpendicular to the surface and having often truncatures which give them the appearance of nearly square pyramids, and the others with the
c axis parallel to the surface.
The oxygen content is evaluated to be
x = 6.97, therefore the formula of the superconducting material could be YBa
2Cu
3O
7. This oxygen amount is relatively homogeneous at various areas on the surface even where the distribution of the crystal aggregate is not homogeneous. After six months, a lost of oxygen, down to
x = 6.8 in the same sample is recorded.
These micro-crystals appear to grow on a continuous ground which was identified as a green phase, Y
2BaCuO
5 resulting from the interaction at the interface between YBa
2Cu
3O
7 and the substrate dopped itself with Y
2O
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2Cu
3O
x deposited on Zirconia (100) substrate, and transiting at 92 K was examined by micro-Raman spectroscopy. The layer is revealed to be an aggregation of two types of micro-crystals: one of them is oriented with the
c axis nearly perpendicular to the surface and having often truncatures which give them the appearance of nearly square pyramids, and the others with the
c axis parallel to the surface.
The oxygen content is evaluated to be
x = 6.97, therefore the formula of the superconducting material could be YBa
2Cu
3O
7. This oxygen amount is relatively homogeneous at various areas on the surface even where the distribution of the crystal aggregate is not homogeneous. After six months, a lost of oxygen, down to
x = 6.8 in the same sample is recorded.
These micro-crystals appear to grow on a continuous ground which was identified as a green phase, Y
2BaCuO
5 resulting from the interaction at the interface between YBa
2Cu
3O
7 and the substrate dopped itself with Y
2O
3.</abstract><cop>Oxford</cop><pub>Elsevier Ltd</pub><doi>10.1016/0038-1098(89)90521-8</doi><tpages>4</tpages></addata></record> |
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issn | 0038-1098 1879-2766 |
language | eng |
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source | Access via ScienceDirect (Elsevier) |
title | Structure and orientation of a superconducting Y-Ba-Cu-O thin film on zirconia substrate. A study by micro-Raman spectroscopy |
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