Zero-energy bound states in superconductor/ferromagnet superlattices
Andreev bound states in monoatomic superconductor–ferromagnet (S/F) superlattices are studied theoretically, assuming tunneling between S and F layers in perpendicular direction. Andreev reflection at S/F interfaces is strongly affected by the exchange interaction h in F layers. In the ground state,...
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Published in | Physica. C, Superconductivity Vol. 320; no. 3; pp. 259 - 266 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
20.07.1999
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Subjects | |
Online Access | Get full text |
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Summary: | Andreev bound states in monoatomic superconductor–ferromagnet (S/F) superlattices are studied theoretically, assuming tunneling between S and F layers in perpendicular direction. Andreev reflection at S/F interfaces is strongly affected by the exchange interaction
h in F layers. In the ground state, only for
h≠0 zero-energy states (ZES) are formed on S and F layers. For
h=0, corresponding to superconductor–normal metal (S/N) superlattices, ZES may appear in the nonequilibrium phase,
ϕ=
π. This is found both for s-wave and d-wave symmetry of the order parameter in S. The conditions for ZES are obtained as a function of
h, of the transfer integral
t for movement of quasiparticles (QPs) between S and F layers, and of the corresponding ground state phase difference
ϕ
e
q
between two neighboring S layers. |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
ISSN: | 0921-4534 1873-2143 |
DOI: | 10.1016/S0921-4534(99)00345-7 |