Electronic anisotropy, magnetic field-temperature phase diagram and their dependence on resistivity in c-axis oriented MgB2 thin films

S. Patnaik; L. D. Cooley; A. Gurevich; A. A. Polyanskii; J. Jiang; X. Y. Cai; A. A. Squitieri; M. T. Naus; M. K. Lee; J. H. Choi; L. Belenky; S. D. Bu; J. Letteri; X. Song; D. G. Schlom; S. E. Babcock; C. B. Eom; E. E. Hellstrom; D. C. Larbalestier

doi:10.1088/0953-2048/14/6/304

arXiv · cond-mat/0104562

Electronic anisotropy, magnetic field-temperature phase diagram and their dependence on resistivity in c-axis oriented MgB2 thin films

S. Patnaik·L. D. Cooley·A. Gurevich·A. A. Polyanskii·J. Jiang·X. Y. Cai·A. A. Squitieri·M. T. Naus·M. K. Lee·J. H. Choi·L. Belenky·S. D. Bu·J. Letteri·X. Song·D. G. Schlom·S. E. Babcock·C. B. Eom·E. E. Hellstrom·D. C. Larbalestier

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Abstract

An important predicted, but so far uncharacterized, property of the new superconductor MgB2 is electronic anisotropy arising from its layered crystal structure. Here we report on three c-axis oriented thin films, showing that the upper critical field anisotropy ratio Hc2par/Hc2perp is 1.8 to 2.0, the ratio increasing with higher resistivity. Measurements of the magnetic field-temperature phase diagram show that flux pinning disappears at H* ~ 0.8Hc2perp(T) in untextured samples. Hc2par(0) is strongly enhanced by alloying to 39 T for the highest resistivity film, more than twice that seen in bulk samples.

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S. Patnaik, L. D. Cooley, A. Gurevich, A. A. Polyanskii, J. Jiang, X. Y. Cai, A. A. Squitieri, M. T. Naus, M. K. Lee, J. H. Choi, L. Belenky, S. D. Bu, J. Letteri, X. Song, D. G. Schlom, S. E. Babcock, C. B. Eom, E. E. Hellstrom, D. C. Larbalestier. 2001-04-28. Electronic anisotropy, magnetic field-temperature phase diagram and their dependence on resistivity in c-axis oriented MgB2 thin films. https://doi.org/10.1088/0953-2048%2F14%2F6%2F304

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