{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:XPBZVHZRGD6Z3F5U3YOYYSAQEA","short_pith_number":"pith:XPBZVHZR","schema_version":"1.0","canonical_sha256":"bbc39a9f3130fd9d97b4de1d8c48102016a8efd1d94c4859c2ff467d243a942c","source":{"kind":"arxiv","id":"0903.0044","version":1},"attestation_state":"computed","paper":{"title":"Origin of the Inverse Spin Switch Effect in Superconducting Spin Valves","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"C. Boone, I. N. Krivorotov, J. Zhu, X. Cheng","submitted_at":"2009-02-28T07:38:55Z","abstract_excerpt":"The resistance of a ferromagnet/superconductor/ferromagnet (F/S/F) spin valve near its superconducting transition temperature, $T_c$, depends on the state of magnetization of the F layers. This phenomenon, known as spin switch effect (SSE), manifests itself as a resistance difference between parallel ($R_P$) and antiparallel ($R_{AP}$) configurations of the F layers. Both standard ($R_{P}>R_{AP}$) and inverse ($R_{P}R_{AP}$) and inverse ($R_{P}