NERNST, SEEBECK, AND HALL-EFFECTS IN THE MIXED-STATE OF YBA2CU3O7-DELTA AND BI2SR2CACU2O8+X THIN-FILMS - A COMPARATIVE-STUDY

被引:141
作者
RI, HC [1 ]
GROSS, R [1 ]
GOLLNIK, F [1 ]
BECK, A [1 ]
HUEBENER, RP [1 ]
WAGNER, P [1 ]
ADRIAN, H [1 ]
机构
[1] TH DARMSTADT, INST FESTKORPERPHYS, D-64289 DARMSTADT, GERMANY
关键词
D O I
10.1103/PhysRevB.50.3312
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The anisotropy of the high-temperature superconductors has strong impact on their transport properties in the mixed state. We have performed a comparative study of the Nernst, Seebeck, and Hall effects of the anisotropic and extremely anisotropic high-temperature superconductors YBa2Cu3O7-delta and Bi2Sr2CaCu2O8+x, respectively. High-quality, c-axis-oriented epitaxial thin films have been used for our study. The temperature and the magnetic-field dependence of the Nernst and Seebeck electric fields were measured both in the mixed state and in the fluctuation regime above the thermodynamic critical temperature. The Seebeck-effect data can be explained well by an extended two-fluid counterflow picture in analogy to the fountain effect in superfluids. From the Nernst-effect data the temperature and magnetic-field dependence of the transport entropy of magnetic-flux lines has been derived. For the magnetic field applied parallel to the c axis of the films, approximately the same value of the transport entropy was found for YBa2Cu3O7-delta and Bi2Sr2CaCu2O8+x, showing that the different anisotropy of these materials has little influence on this quantity. From our experimental data in the mixed state and the fluctuation regime well above the mean-field critical temperature, the upper-critical-field slope was derived. For both regimes, dH(c2)/dT = -2.4 +/- 0.2 and -2.5 +/- 0.2 T/K for YBa2Cu3O7-delta and Bi2Sr2CaCu2O8+x, corresponding to a Ginzburg-Landau coherence length xi(ab) = 14.5 and 14.2 angstrom, respectively. The Hall resistivity rho(xy) of both materials showed a sign anomaly in the mixed state and scaled with the longitudinal resistivity rho(xx) as rho(xy)(T) = K-1rho(xx)beta (T) with beta congruent-to 2 and a magnetic-field-independent coefficient K.
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收藏
页码:3312 / 3329
页数:18
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