Coulomb blockade in a quantum wire with long-range interactions

Europhysics Letters

Volumn 38, Issue 9, 1997, Pages 681-686

  Maurey, H ^a,b   Giamarchi, T ^a  

^a UNIVERSITÉ PARIS SUD   (France)

^b JOHNS HOPKINS UNIVERSITY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0031580160     PISSN: 02955075     EISSN: None     Source Type: Journal    
DOI: 10.1209/epl/i1997-00303-0     Document Type: Article

References (31)

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26. 2/h per channel, not renormalized by the interactions, contrary to previous predictions. (KAWABATA A., J. Phys. Soc. Jpn., 65 (1996) 30; OREG Y. and FINKEL'STEIN A. M., Phys. Rev. B, 54 (1996) R14265. See also SAFI I. and SCHULZ H. J., Phys. Rev. B, 52 (1995) R17040; MASLOV D. and STONE M., Phys. Rev. B, 52 (1995) R5539). However, this effect does not change the T-dependence of the leading corrections δG, which are merely multiplied by a factor of order 1. Thus using Kubo formula is sufficient for our purpose. This is still valid for the small G(T) in the strong impurity case.
27. 2/h per channel, not renormalized by the interactions, contrary to previous predictions. (KAWABATA A., J. Phys. Soc. Jpn., 65 (1996) 30; OREG Y. and FINKEL'STEIN A. M., Phys. Rev. B, 54 (1996) R14265. See also SAFI I. and SCHULZ H. J., Phys. Rev. B, 52 (1995) R17040; MASLOV D. and STONE M., Phys. Rev. B, 52 (1995) R5539). However, this effect does not change the T-dependence of the leading corrections δG, which are merely multiplied by a factor of order 1. Thus using Kubo formula is sufficient for our purpose. This is still valid for the small G(T) in the strong impurity case.
28. 2/h per channel, not renormalized by the interactions, contrary to previous predictions. (KAWABATA A., J. Phys. Soc. Jpn., 65 (1996) 30; OREG Y. and FINKEL'STEIN A. M., Phys. Rev. B, 54 (1996) R14265. See also SAFI I. and SCHULZ H. J., Phys. Rev. B, 52 (1995) R17040; MASLOV D. and STONE M., Phys. Rev. B, 52 (1995) R5539). However, this effect does not change the T-dependence of the leading corrections δG, which are merely multiplied by a factor of order 1. Thus using Kubo formula is sufficient for our purpose. This is still valid for the small G(T) in the strong impurity case.
29. 2/h per channel, not renormalized by the interactions, contrary to previous predictions. (KAWABATA A., J. Phys. Soc. Jpn., 65 (1996) 30; OREG Y. and FINKEL'STEIN A. M., Phys. Rev. B, 54 (1996) R14265. See also SAFI I. and SCHULZ H. J., Phys. Rev. B, 52 (1995) R17040; MASLOV D. and STONE M., Phys. Rev. B, 52 (1995) R5539). However, this effect does not change the T-dependence of the leading corrections δG, which are merely multiplied by a factor of order 1. Thus using Kubo formula is sufficient for our purpose. This is still valid for the small G(T) in the strong impurity case.
30. i their density [12]. (See GIAMARCHI T. and MAUREY H., in Correlated Fermions and Transport in Mesoscopic Systems, edited by G. MONTAMBAUX et al. (Editions Frontières, Gif-sur-Yvette) 1996.)
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