메뉴 건너뛰기




Volumn 61, Issue 22, 2000, Pages 15370-15381

Strong-coupling limit in the evolution from BCS superconductivity to Bose-Einstein condensation

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0000710557     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.61.15370     Document Type: Article
Times cited : (202)

References (29)
  • 4
    • 0039224686 scopus 로고    scopus 로고
    • A. G. Loeser et. al Science 273, 325 (1996).
    • (1996) Science , vol.273 , pp. 325
    • Loeser, A.1
  • 6
    • 0001020566 scopus 로고
    • V. M. Galitskii, Zh. Éksp. Teor. Fiz. 34, 151 (1958) [Sov. Phys. JETP 7, 104 (1958)].
    • (1958) Sov. Phys. JETP , vol.7 , pp. 104
    • Galitskii, V.1
  • 7
    • 0000724476 scopus 로고
    • S. T. Beliaev, Zh. Éksp. Teor. Fiz. 34, 433 (1958) [Sov. Phys. JETP 7, 299 (1958)].
    • (1958) Sov. Phys. JETP , vol.7 , pp. 299
    • Beliaev, S.1
  • 17
    • 0031633269 scopus 로고    scopus 로고
    • Already at the mean-field level, the exact solution available for a contact potential [M. Marini, F. Pistolesi, and G. C. Strinati, Eur. Phys. J. B 1, 151 (1998)] shows that approximations valid on the BE side extrapolate well to the BCS side, but not vice versa.
    • (1998) Eur. Phys. J. B , vol.1 , pp. 151
    • Marini, M.1    Pistolesi, F.2    Strinati, G.3
  • 18
    • 0001016153 scopus 로고    scopus 로고
    • The choice of the “contact” potential (2.2) does not allow the fermionic attraction to extend over a finite range. If a finite-range fermionic attraction would instead have been adopted, the effective boson-boson potential in the strong-coupling limit would acquire an attractive part which would dominate over the usual repulsive part due to Pauli principle, in the sense that the bosonic scattering length associated with the attractive part would not vanish in that limit. The attractive part would thus lead to an instability of the bosonic system when the finite-range fermionic attraction gets sufficiently strong. To avoid this instability, a condition of the type (Formula presented) has to be imposed on the BE limit, where (Formula presented) is the wave vector specifying the finite range of the potential and (Formula presented) is the bound-state energy of the two-body problem [cf. footnote 43 of Ref. 15]. In this context, it is worth mentioning the recent work by G. Röpke et. al [Phys. Rev. Lett. 80, 3177 (1998)] where it has been shown that, in the strong-coupling limit, there exists a competition between pair and quartet condensation in a Fermi liquid with finite-range attraction. It is then clear that adopting a finite-range fermionic potential merely makes the BCS-BE crossover more involved, and it is thus not relevant to the purposes of the present paper.
    • (1998) Phys. Rev. Lett. , vol.80 , pp. 3177
    • Röpke, G.1
  • 23
    • 33748957360 scopus 로고
    • G. Baym, Phys. Rev. 127, 1391 (1962).
    • (1962) Phys. Rev. , vol.127 , pp. 1391
    • Baym, G.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.