Matches in SemOpenAlex for { <https://semopenalex.org/work/W2018314610> ?p ?o ?g. }
- W2018314610 abstract "We study a tunnel junction consisting of two thin-film $s$-wave superconductors separated by a thin, insulating barrier in the presence of misaligned in-plane exchange fields. We find an interesting interplay between the superconducting phase difference and the relative orientation of the exchange fields, manifested in the Josephson current across the junction. Specifically, this may be written ${I}_{mathrm{J}}^{mathrm{C}}=({I}_{0}+{I}_{m}phantom{rule{0.2em}{0ex}}mathrm{cos}phantom{rule{0.2em}{0ex}}ensuremath{varphi})mathrm{sin}phantom{rule{0.2em}{0ex}}ensuremath{Delta}ensuremath{theta}$, where ${I}_{0}$ and ${I}_{m}$ are constants, and $ensuremath{varphi}$ is the relative orientation of the exchange fields, while $ensuremath{Delta}ensuremath{theta}$ is the superconducting phase difference. Similar results have recently been obtained in other superconductor-insulator-superconductor junctions coexisting with helimagnetic or ferromagnetic order. We calculate the superconducting order parameter self-consistently, and investigate quantitatively the effect which the misaligned exchange fields constitute on the Josephson current, to see if ${I}_{m}$ may have an appreciable effect on the Josephson current. It is found that ${I}_{0}$ and ${I}_{m}$ become comparable in magnitude at sufficiently low temperatures and fields close to the critical value, in agreement with previous work. From our analytical results, it then follows that the Josephson current in the present system may be controlled in a well-defined manner by a rotation of the exchange fields on both sides of the junction. We discuss a possible experimental realization of this proposition." @default.
- W2018314610 created "2016-06-24" @default.
- W2018314610 creator A5036914810 @default.
- W2018314610 creator A5052287133 @default.
- W2018314610 date "2007-08-20" @default.
- W2018314610 modified "2023-10-10" @default.
- W2018314610 title "Josephson effect in thin-film superconductor/insulator/superconductor junctions with misaligned in-plane magnetic fields" @default.
- W2018314610 cites W1590432413 @default.
- W2018314610 cites W1673591018 @default.
- W2018314610 cites W1677435873 @default.
- W2018314610 cites W1971087148 @default.
- W2018314610 cites W1972359105 @default.
- W2018314610 cites W1976175889 @default.
- W2018314610 cites W1987598609 @default.
- W2018314610 cites W1989116198 @default.
- W2018314610 cites W1991852719 @default.
- W2018314610 cites W1996316408 @default.
- W2018314610 cites W1998444730 @default.
- W2018314610 cites W2014437371 @default.
- W2018314610 cites W2019181508 @default.
- W2018314610 cites W2020517872 @default.
- W2018314610 cites W2027456087 @default.
- W2018314610 cites W2027592739 @default.
- W2018314610 cites W2031702142 @default.
- W2018314610 cites W2037707262 @default.
- W2018314610 cites W2041923345 @default.
- W2018314610 cites W2042473487 @default.
- W2018314610 cites W2053739713 @default.
- W2018314610 cites W2054753178 @default.
- W2018314610 cites W2056078006 @default.
- W2018314610 cites W2060002594 @default.
- W2018314610 cites W2061382801 @default.
- W2018314610 cites W2062976961 @default.
- W2018314610 cites W2064077602 @default.
- W2018314610 cites W2069604995 @default.
- W2018314610 cites W2070278064 @default.
- W2018314610 cites W2070812785 @default.
- W2018314610 cites W2072509738 @default.
- W2018314610 cites W2072700116 @default.
- W2018314610 cites W2073732631 @default.
- W2018314610 cites W2074689366 @default.
- W2018314610 cites W2076376389 @default.
- W2018314610 cites W2081628261 @default.
- W2018314610 cites W2082968079 @default.
- W2018314610 cites W2085594085 @default.
- W2018314610 cites W2087845030 @default.
- W2018314610 cites W2088633776 @default.
- W2018314610 cites W2090132933 @default.
- W2018314610 cites W2131974386 @default.
- W2018314610 cites W2152466677 @default.
- W2018314610 cites W2152989635 @default.
- W2018314610 cites W2163120301 @default.
- W2018314610 cites W3098072010 @default.
- W2018314610 cites W3143371796 @default.
- W2018314610 cites W4233753848 @default.
- W2018314610 cites W4237044745 @default.
- W2018314610 cites W4239959335 @default.
- W2018314610 cites W4247777445 @default.
- W2018314610 cites W4256151410 @default.
- W2018314610 doi "https://doi.org/10.1103/physrevb.76.064524" @default.
- W2018314610 hasPublicationYear "2007" @default.
- W2018314610 type Work @default.
- W2018314610 sameAs 2018314610 @default.
- W2018314610 citedByCount "12" @default.
- W2018314610 countsByYear W20183146102014 @default.
- W2018314610 countsByYear W20183146102015 @default.
- W2018314610 countsByYear W20183146102019 @default.
- W2018314610 crossrefType "journal-article" @default.
- W2018314610 hasAuthorship W2018314610A5036914810 @default.
- W2018314610 hasAuthorship W2018314610A5052287133 @default.
- W2018314610 hasBestOaLocation W20183146102 @default.
- W2018314610 hasConcept C10138342 @default.
- W2018314610 hasConcept C12038964 @default.
- W2018314610 hasConcept C121332964 @default.
- W2018314610 hasConcept C162324750 @default.
- W2018314610 hasConcept C16345878 @default.
- W2018314610 hasConcept C180349316 @default.
- W2018314610 hasConcept C182306322 @default.
- W2018314610 hasConcept C212702 @default.
- W2018314610 hasConcept C2524010 @default.
- W2018314610 hasConcept C26873012 @default.
- W2018314610 hasConcept C2987373456 @default.
- W2018314610 hasConcept C3017413879 @default.
- W2018314610 hasConcept C33923547 @default.
- W2018314610 hasConcept C44280652 @default.
- W2018314610 hasConcept C49040817 @default.
- W2018314610 hasConcept C54101563 @default.
- W2018314610 hasConcept C62520636 @default.
- W2018314610 hasConcept C94715708 @default.
- W2018314610 hasConceptScore W2018314610C10138342 @default.
- W2018314610 hasConceptScore W2018314610C12038964 @default.
- W2018314610 hasConceptScore W2018314610C121332964 @default.
- W2018314610 hasConceptScore W2018314610C162324750 @default.
- W2018314610 hasConceptScore W2018314610C16345878 @default.
- W2018314610 hasConceptScore W2018314610C180349316 @default.
- W2018314610 hasConceptScore W2018314610C182306322 @default.
- W2018314610 hasConceptScore W2018314610C212702 @default.
- W2018314610 hasConceptScore W2018314610C2524010 @default.
- W2018314610 hasConceptScore W2018314610C26873012 @default.
- W2018314610 hasConceptScore W2018314610C2987373456 @default.