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Volumn 59, Issue 2, 1999, Pages 1354-1357

Superconductivity from a pseudogapped normal state: a mode-coupling approach to precursor superconductivity

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EID: 0346966564     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.59.1354     Document Type: Article
Times cited : (86)

References (24)
  • 1
    • 85038279584 scopus 로고    scopus 로고
    • P. W. Anderson, The Theory of Superconductivity in the High-(Formula presented) Cuprate Superconductors (Princeton University Press, Princeton, 1997)
    • P. W. Anderson, The Theory of Superconductivity in the High-(Formula presented) Cuprate Superconductors (Princeton University Press, Princeton, 1997).
  • 14
    • 85038320931 scopus 로고    scopus 로고
    • We thank Ioan Kosztin and Qinjin Chen for pointing out these 2D results
    • We thank Ioan Kosztin and Qinjin Chen for pointing out these 2D results.
  • 16
    • 85038331225 scopus 로고    scopus 로고
    • While we consider the s-wave symmetry case, d-wave symmetry can be readily introduced via the (Formula presented) and in the 2D limit
    • While we consider the s-wave symmetry case, d-wave symmetry can be readily introduced via the (Formula presented) and in the 2D limit.
  • 17
    • 85038306993 scopus 로고    scopus 로고
    • B. R. Patton, Ph.D. thesis, Cornell University, 1971
    • B. R. Patton, Ph.D. thesis, Cornell University, 1971.
  • 18
    • 33646515721 scopus 로고
    • The detailed form used here for the T matrix is more readily related to that in Ref. 13 than in Ref. 8. It should also be noted that we have verified that this diagrammatic scheme is consistent with the general criteria for number conservation in G. Baym and L. P. Kadanoff, Phys. Rev. 124, 287 (1961).
    • (1961) Phys. Rev. , vol.124 , pp. 287
    • Baym, G.1    Kadanoff, L.P.2
  • 19
    • 85038346240 scopus 로고    scopus 로고
    • Here we have dropped a structureless term which may be parametrized as (Formula presented) This is relatively unimportant when the self-energy is integrated over, as in computing (Formula presented) However, it will contribute to properties such as the density of states where it is necessary to regularize the self-energy so that it is never a strict delta function in the normal state
    • Here we have dropped a structureless term which may be parametrized as (Formula presented) This is relatively unimportant when the self-energy is integrated over, as in computing (Formula presented) However, it will contribute to properties such as the density of states where it is necessary to regularize the self-energy so that it is never a strict delta function in the normal state.
  • 22
    • 85038332782 scopus 로고    scopus 로고
    • It should also be noted that the imaginary part of (Formula presented) vanishes at (Formula presented) Moreover, in numerical iterations, expecially near (Formula presented) a Landau-Ginzburg (small (Formula presented) expansion was used to simplify various integrals
    • It should also be noted that the imaginary part of (Formula presented) vanishes at (Formula presented) Moreover, in numerical iterations, expecially near (Formula presented) a Landau-Ginzburg (small (Formula presented) expansion was used to simplify various integrals.
  • 23
    • 0001051342 scopus 로고    scopus 로고
    • Pseudogap effects are expected to increase, as the insulator is approached, as a consequence of a three- to two-dimensional crossover, as well as a reduction in the plasma frequency; see J. Maly, K. Levin, and D. Z. Liu, Phys. Rev. B 54, 15 657 (1996).
    • (1996) Phys. Rev. B , vol.54 , pp. 15
    • Maly, J.1    Levin, K.2    Liu, D.Z.3
  • 24
    • 85038267887 scopus 로고    scopus 로고
    • (unpublished)
    • M. Norman (unpublished).
    • Norman, M.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.