Hostname: page-component-78c5997874-v9fdk Total loading time: 0 Render date: 2024-11-19T07:10:45.643Z Has data issue: false hasContentIssue false

Synthesis and Superconducting Properties of Metastable Y(Ba2−xYx)Cu3O7+δ

Published online by Cambridge University Press:  28 February 2011

Z. Iqbal
Affiliation:
Allied-Signal Inc., Corporate Technology, Morristown, N.J. 07960U.S.A.
F. Reidinger
Affiliation:
Allied-Signal Inc., Corporate Technology, Morristown, N.J. 07960U.S.A.
A. Bose
Affiliation:
Allied-Signal Inc., Corporate Technology, Morristown, N.J. 07960U.S.A.
N. Cipollini
Affiliation:
Allied-Signal Inc., Corporate Technology, Morristown, N.J. 07960U.S.A.
H. Eckhardt
Affiliation:
Allied-Signal Inc., Corporate Technology, Morristown, N.J. 07960U.S.A.
B. L. Ramakrishna
Affiliation:
Department of Chemistry, Arizona State University, Tempe, AZ 85287, U.S.A.
E. W. Ong
Affiliation:
Department of Chemistry, Arizona State University, Tempe, AZ 85287, U.S.A.
Get access

Abstract

The oxygen-deficient orthorhombic oxide YBa2Cu3O7-δ has been the center of intense recent interest because of its high Tc superconducting proper-ties[l-3]. Recently, the structurally related La3Ba3Cu3O15-δ, has received increasing attention[4–9]. The pure Y analog[10,11] cannot be synthesized by usual solid state reaction routes probably because of its metastability near 880°C. Here we report on the successful synthesis of pure tetragonal Y3,Ba3CU6O15-δ (referred to as Y 3–3–6), via the firing of an atomically mixed citrate precursor at a relatively low temperature. X-ray diffraction data characterize Y 3–3–6 to be isostructural with the corresponding La compound[4]. The unit cell composition can then be written as: Y(Ba2−x Yx) CU3O7+δ with the parent compound at x = 0.50. Specimens of Y 3–3–6 at × = 0.50 and 0.375 annealed at 650°C under 1 atmosphere of O2 are non-superconducting. Higher pressure O2 annealing and fluorine-doping leads to a 1–5% superconducting volume fraction with onset at 85K. Annealing near 880°C creates a 10% superconducting fraction which shows near-zero resistivity at 62K and a reproducible, small resistive transition near 260K.

Type
Research Article
Copyright
Copyright © Materials Research Society 1988

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

1. Wu, M.K., et al., Phys. Rev. Lett. 58, 908911 (1987).Google Scholar
2. David, W.I.F., et al., Nature 327, 310312 (1987).Google Scholar
3. Siegrist, T., et al., Phys. Rev. B35, 71377140 (1987).Google Scholar
4. David, W.I.F., et al., Nature 328, 328329 (1987).Google Scholar
5. Attfield, J.P., et al., submitted to Nature, August 28 (1987).Google Scholar
6. Torardi, C.C., et al., Mater. Res. Bull. - in press.Google Scholar
7. Mitzi, D.B., et al., Phys. Rev. B (submitted).Google Scholar
8. Maeda, A., et al., Jap. J. Appl. Phys. 26, L1366 (1987).Google Scholar
9. CSegre, U., et al., Nature 329, 227229 (1987).Google Scholar
10. Er-Rakho, L., et al., Solid State Chem. 37, 151156 (1981).Google Scholar
11. Rao, C.N.R., et al., Nature 326, 856857 (1987).Google Scholar