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Thermally activated dissipation and irreversibility fields of bismuth oxide superconductors

H. Yamasaki, K. Endo, S. Kosaka, M. Umeda, S. Yoshida, K. Kajimura

DOI 10.1103/PhysRevB.49.6913 · Physical Review B

T1

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Abstract

Thermally activated dissipation is investigated in epitaxial Bi-2:2:2:3 films in magnetic fields parallel to the c axis. For a wide temperature T and field B range the resistivity ρ shows clear Arrhenius behavior with an activation energy U0=A(1-T/Tc)/ √B : ρ(B,T)=ρ0exp(-U0/kT)=ρ0exp[-A(1-T/ Tc)/kT √B ], which is explained by thermally activated flux motion with the formation of double kinks. Temperature dependence of the irreversibility field B* is predicted by flux-creep theory as √B* =C(1/kT-1/kTc), when B* is defined by an electric-field criterion. This relation holds not only for our films but also for magnetically determined B* of Bi-2:2:2:3 samples, which suggests that the irreversibility line originates from thermally activated plastic motion of pinned flux liquid.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Bi2Sr2Ca2Cu3O

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110Pressure not reportedonset
Bi2Sr2Ca2Cu3O

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100Pressure not reportedmidpoint
Bi2Sr2Ca2Cu3O

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86.5Pressure not reportedzero_resistance
Bi2Sr2CaCu2Ox

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—Pressure not reportedunknown
YBa2Cu3O7

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—Pressure not reportedunknown
(La,Ba)2CuO4

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—Pressure not reportedunknown

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