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Volumn 67, Issue 1, 2003, Pages

Universality of delocalization in unconventional dirty superconducting wires with broken spin-rotation symmetry

Author keywords

[No Author keywords available]

Indexed keywords

METAL;

EID: 0037281972     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.67.014530     Document Type: Article
Times cited : (42)

References (22)
  • 13
    • 0002448247 scopus 로고
    • Interestingly, the thick-wire limit is a necessary step in the derivation of the one-dimensional nonlinear sigma model, see, e.g., and
    • Interestingly, the thick-wire limit is a necessary step in the derivation of the one-dimensional nonlinear sigma model, see, e.g., A D. Mirlin, A. Müller-Groeling, and M R. Zirnbauer, Ann. Phys. (N.Y.)236, 325 (1994).
    • (1994) Ann. Phys. (N.Y.) , vol.236 , pp. 325
    • Mirlin, A.D.1    Müller-Groeling, A.2    Zirnbauer, M.R.3
  • 14
    • 0001484848 scopus 로고    scopus 로고
    • The Fokker-Planck approach is often used without the thick-wire limit, though equivalence of the Fokker-Planck and field-theoretic approach is only established if the thick-wire limit is taken; see, and
    • The Fokker-Planck approach is often used without the thick-wire limit, though equivalence of the Fokker-Planck and field-theoretic approach is only established if the thick-wire limit is taken; see P W. Brouwer and K M. Frahm, Phys. Rev. B53, 1490 (1996).
    • (1996) Phys. Rev. B , vol.53 , pp. 1490
    • Brouwer, P.W.1    Frahm, K.M.2
  • 15
    • 0000197543 scopus 로고    scopus 로고
    • To illustrate this point, note that an infinitesimal magnetic field already changes the, of the Hamiltonian from orthogonal to unitary. However, for a wire of finite thickness, one needs a finite magnetic field to reach the unitary class, while in the thick-wire limit an infinitesimal field is sufficient. See, e.g., and
    • To illustrate this point, note that an infinitesimal magnetic field already changes the symmetry of the Hamiltonian from orthogonal to unitary. However, for a wire of finite thickness, one needs a finite magnetic field to reach the unitary class, while in the thick-wire limit an infinitesimal field is sufficient. See, e.g., H. Schomerus and C W J. Beenakker, Phys. Rev. Lett.84, 3927 (2000).
    • (2000) Phys. Rev. Lett. , vol.84 , pp. 3927
    • Schomerus, H.1    Beenakker, C.W.J.2
  • 20
    • 85038299899 scopus 로고    scopus 로고
    • For (formula presented) or (formula presented) the class D result (4) is obtained already for wire lengths, of the order of the mean free path
    • For (formula presented) or (formula presented) the class D result (4) is obtained already for wire lengths L of the order of the mean free path.
  • 21
    • 85038342644 scopus 로고    scopus 로고
    • Note that the limit (formula presented) of the scaling function (formula presented) is a different quantity than the limit (formula presented) of the Lyapunov exponent, which is defined by taking the limit (formula presented), the limit (formula presented) in Eq. (8)
    • Note that the limit (formula presented) of the scaling function (formula presented) is a different quantity than the limit (formula presented) of the Lyapunov exponent, which is defined by taking the limit (formula presented) before the limit (formula presented) in Eq. (8).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.