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Volumn 308, Issue 1, 2003, Pages 156-200

Conductance distribution in quasi-one-dimensional disordered quantum wires

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EID: 0344152919     PISSN: 00034916     EISSN: None     Source Type: Journal    
DOI: 10.1016/S0003-4916(03)00136-2     Document Type: Article
Times cited : (35)

References (42)
  • 9
    • 0037041075 scopus 로고    scopus 로고
    • The importance of electron-electron interactions in the distribution has recently been pointed out in Unfortunately, it is not possible to include interaction effects on the full P(g) at all disorder within any framework known today
    • The importance of electron-electron interactions in the distribution has recently been pointed out in P. Mohanty and R.A. Webb, Phys. Rev. Lett. 88 (2002) 146601. Unfortunately, it is not possible to include interaction effects on the full P(g) at all disorder within any framework known today.
    • (2002) Phys. Rev. Lett. , vol.88 , pp. 146601
    • Mohanty, P.1    Webb, R.A.2
  • 15
    • 85030951327 scopus 로고    scopus 로고
    • cond-mat/0211037
    • P. Markoš, cond-mat/0211037.
    • Markoš, P.1
  • 21
    • 0039086538 scopus 로고
    • Exact distribution for 1d conductors is known, see e.g., but there is no metallic regime in 1d. The 3rd cumulant of the distribution has been obtained for quasi-1D systems using random matrix theory by A.M. Macedo (Phys. Rev. B 49 (1994) 1858) and by V.A. Gopar, M. Martinez, and P.A. Mello Phys. Rev. B 51 (1995) and using a scaling method by A.V. Tartakovski (Phys. Rev. B 52 (1995) 2704). It has also been calculated for weak disorder in higher dimensions within standard perturbation theory by M.C. van Rossum et al. (Phys. Rev. B 55 (1997) 4710)
    • Exact distribution for 1d conductors is known, see e.g., B.L. Altshuler and V.N. Prigodin, JETP Lett. 45 (1987) 687, but there is no metallic regime in 1d. The 3rd cumulant of the distribution has been obtained for quasi-1D systems using random matrix theory by A.M. Macedo (Phys. Rev. B 49 (1994) 1858) and by V.A. Gopar, M. Martinez, and P.A. Mello Phys. Rev. B 51 (1995) and using a scaling method by A.V. Tartakovski (Phys. Rev. B 52 (1995) 2704). It has also been calculated for weak disorder in higher dimensions within standard perturbation theory by M.C. van Rossum et al. (Phys. Rev. B 55 (1997) 4710).
    • (1987) JETP Lett. , vol.45 , pp. 687
    • Altshuler, B.L.1    Prigodin, V.N.2
  • 38
    • 0004163930 scopus 로고
    • second ed., Academic Press, New York
    • M.L Mehta, Random Matrices, second ed., Academic Press, New York, 1991.
    • (1991) Random Matrices
    • Mehta, M.L.1
  • 41
    • 0037105082 scopus 로고    scopus 로고
    • A generalized phenomenological DMPK equation has recently been proposed by
    • A generalized phenomenological DMPK equation has recently been proposed by K.A. Muttalib and V.A. Gopar, Phys. Rev. B 66 (2002) 115318.
    • (2002) Phys. Rev. B , vol.66 , pp. 115318
    • Muttalib, K.A.1    Gopar, V.A.2


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.