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Volumn 52, Issue 5, 1995, Pages 3087-3090

Josephson current-phase relationships with unconventional superconductors

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0000744452     PISSN: 01631829     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevB.52.3087     Document Type: Article
Times cited : (123)

References (20)
  • 11
    • 84927999326 scopus 로고    scopus 로고
    • Notice now since I( chi) is nonsinusoidal, the current phase relationship of a chim junction is in general not given by that of a 0 junction shifted by chim.
  • 12
    • 84927999325 scopus 로고    scopus 로고
    • For tunneling along hat z between an s wave and B1g superconductors occupying z > < 0, the result that one has a π/2 junction is actually implicit in, Ref. 13
  • 14
    • 84927999324 scopus 로고    scopus 로고
    • This in fact corresponds to the situation in the microscopic calculations below. I shall not discuss the other cases due to the lack of space.
  • 15
    • 84927999323 scopus 로고    scopus 로고
    • I have been unable to prove analytically whether it is actually a straight line.
  • 19
    • 84927999321 scopus 로고    scopus 로고
    • In the tunnel junction limit the flux will not exist at a corner unless one of the interfaces is a 0 junction and the other a π junction, and in that case the flux generated will be Φo over 2, whereas there will be no fluxes along a planar interface, both contrary to the observations, Ref. 18
  • 20
    • 84927999320 scopus 로고    scopus 로고
    • A rather different explanation involving broken time reversal symmetry has been advanced recently by Sigrist et al., Phys. Rev. Lett. 74, 3249 (1995).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.