π phase in magnetic-layered superconductors
A. V. Andreev, A. I. Buzdin, R. M. Osgood, III
DOI 10.1103/PhysRevB.43.10124 · Physical Review B
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Abstract
We show that in a system composed of alternating superconducting and magnetic layers the ground state may be the so-called ‘‘π phase,’’ wherein the superconducting order parameter changes its sign as we go from one superconducting layer to another. This phase is similar to the Larkin-Ovchinnikov-Fulde-Ferrell phase. We find that the π phase exists, under certain conditions, in the presence of both ferro- and antiferromagnetism.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| RBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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