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Anomaly of zero-bias conductance peaks in ferromagnet/d-wave superconductor junctions

Z. C. Dong, D. Y. Xing, Z. D. Wang, Ziming Zheng, Jinming Dong

DOI 10.1103/PhysRevB.63.144520 · Physical Review B

T1

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Abstract

The Blonder-Tinkham-Klapwijk approach is applied to studying spin-polarized quasiparticle transport in ferromagnet (FM)/d-wave superconductor (SC) junctions by taking into account the roughness of the interfacial barrier, broken time-reversal symmetry (BTRS) states near the surface of the SC, and exchange interactions in the FM. It is shown that (1) the exchange splitting in the FM decreases the height of the zero-bias conductance peak (ZBCP) and may induce a zero-bias conductance dip (ZBCD), (2) the presence of the BTRS states in the SC may make the ZBCP split into two peaks, and (3) the interface roughness obstructs the ZBCP splitting and decreases the height of the ZBCP. The calculated results can account for the ZBCD observed experimentally in La2/3Ba1/3MnO3/DyBa2Cu3O7 and La2/3Ba1/3MnO3/YBa2Cu3O7−δ junctions.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
La2/3Ba1/3MnO3/DyBa2Cu3O7

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—Pressure not reportedunknown
La2/3Ba1/3MnO3/YBa2Cu3O7-δ

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—Pressure not reportedunknown
YBa2Cu3O7

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—Pressure not reportedunknown
Tl2Ba2CaCu2O

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—Pressure not reportedunknown
Bi2Sr2CaCu2O8

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—Pressure not reportedunknown
La1.85Sr0.15CuO4

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—Pressure not reportedunknown

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