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High-Field Quasiparticle Tunneling in Bi2Sr2CaCu2O8+δ: Negative Magnetoresistance in the Superconducting State

N. Morozov, L. Krusin-Elbaum, T. Shibauchi, L. N. Bulaevskii, M. P. Maley, Yu. I. Latyshev, T. Yamashita

DOI 10.1103/PhysRevLett.84.1784 · Physical Review Letters

T1

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Abstract

We report on the c-axis resistivity ρc(H) in Bi2Sr2CaCu2O8+δ that peaks in quasistatic magnetic fields up to 60 T. By suppressing the Josephson part of the two-channel (Cooper pair/quasiparticle) conductivity σc(H), we find that the negative slope of ρc(H) above the peak is due to quasiparticle tunneling conductivity σq(H) across the CuO2 layers below Hc2. At high fields (a) σq(H) grows linearly with H, and (b) ρc(T) tends to saturate ( σc≠0) as T→0, consistent with the scattering at the nodes of the d-wave gap. A superlinear σq(H) marks the normal state above Tc.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Bi2Sr2CaCu2O8+δ

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92.5Pressure not reportedunknown
Bi2Sr2CaCu2O8+δ

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

89Pressure not reportedunknown
YBa2Cu3O7-δ

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown

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