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Extension of the 3D-scaling rule for resistivity as a function of magnetic field and its orientation for anisotropic high-temperature superconductors

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Abstract

The measurement of the c-axis resistivity of single crystalline La1.86Sr0.14CuO4 is performed at different constant temperatures as a function of magnetic field H and angle θ between H and the ab-plane. It is shown that the 2D- or 3D-scaling rule proposed for high-T c superconductors does not work well for the present system. Taking into account unusual vortex dynamics in the high-T c systems, an extension is made to the 3D-scaling rule developed on the basis of the effective-mass model. Based on this extended rule, it is shown that at each given temperature the observed resistivity as a function of H and θ could be consistently scaled onto the corresponding Lorentz-force-free magnetoresistivity curves directly measured in H‖I‖c.

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Author notes

  1. Z. J. Yang

    Present address: Department of Physics, Dalhousie University, B3H 3J5, Halifax, NS, Canada

Authors and Affiliations

  1. High Magnetic Field Laboratory, Institute of Plasma Physics, Academia Sinica, 230031, Hefei, People's Republic of China

    S. L. Yuan, J. Q. Li, Z. Huang, J. L. Chen & B. J. Gao

  2. Department of Industrial Chemistry, University of Tokyo, 7-3-1 Hongo, 113, Tokyo, Japan

    Z. J. Yang, T. Kimura & K. Kishio

  3. National Research Institute for Metals, Tsukuba Laboratory, 305, Ibaraki, Japan

    K. Kadowaki

Authors
  1. S. L. Yuan
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  2. Z. J. Yang
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  3. K. Kadowaki
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  4. J. Q. Li
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  5. T. Kimura
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  6. K. Kishio
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  7. Z. Huang
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  8. J. L. Chen
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  9. B. J. Gao
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Additional information

On leave from Department of Physics, Wuhan Institute of Technology, Wuhan, People's Republic of China

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Yuan, S.L., Yang, Z.J., Kadowaki, K. et al. Extension of the 3D-scaling rule for resistivity as a function of magnetic field and its orientation for anisotropic high-temperature superconductors. Appl. Phys. A 59, 583–587 (1994). https://doi.org/10.1007/BF00331916

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  • DOI: https://doi.org/10.1007/BF00331916

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