Change of strength of vortex pinning in YBCO due to BaZrO3 inclusions
We probe the short-range pinning properties with the application of microwave currents at very high driving frequencies (47.7GHz) on YBa2Cu3O7−δ films with and without sub-micrometer BaZrO3 inclusions. We explore the temperature and field ranges 60 K <T<Tc and 0<μ0H<0.8T, with the field...
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Published in: | Physica. C, Superconductivity Vol. 468; no. 7-10; pp. 745 - 748 |
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Main Authors: | , , , , |
Format: | Journal Article Conference Proceeding |
Language: | English |
Published: |
Amsterdam
Elsevier B.V
01-04-2008
Elsevier Science |
Subjects: | |
Online Access: | Get full text |
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Summary: | We probe the short-range pinning properties with the application of microwave currents at very high driving frequencies (47.7GHz) on YBa2Cu3O7−δ films with and without sub-micrometer BaZrO3 inclusions. We explore the temperature and field ranges 60 K <T<Tc and 0<μ0H<0.8T, with the field applied along the c-axis. The magnetic field induces a much smaller increase of the microwave resistivity, Δρ1(H)+iΔρ2(H), in YBa2Cu3O7−δ/BaZrO3 with respect to pure YBa2Cu3O7−δ. Δρ1(H) is slightly superlinear in pure YBa2Cu3O7−δ (suggesting a possible contribution of thermal activation), but linear or sublinear in YBa2Cu3O7−δ/BaZrO3 (suggesting a possible suppression of thermal activation as a consequence of BaZrO3 inclusions). These features persist up to close to Tc. We discuss our data in terms of the ratio r=Δρ2(H)/Δρ1(H) in the framework of the models for the microwave surface impedance in the mixed state. Large r are found in YBa2Cu3O7−δ/BaZrO3, with little field dependence. By contrast, smaller values and stronger field dependences are found in pure YBa2Cu3O7−δ. We discuss the different field dependence of the pinning constant. |
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Bibliography: | SourceType-Scholarly Journals-2 ObjectType-Feature-2 ObjectType-Conference Paper-1 content type line 23 SourceType-Conference Papers & Proceedings-1 ObjectType-Article-3 |
ISSN: | 0921-4534 1873-2143 |
DOI: | 10.1016/j.physc.2007.11.040 |