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7
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33644909733
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D.M. Basko, I.L. Aleiner, B.L. Altshuler; e-print arXiv:cond-mat/0506617
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D.M. Basko, I.L. Aleiner, B.L. Altshuler; e-print arXiv:cond-mat/0506617
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10
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33644917848
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The dimension 1 is special, see reference [14] for details
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The dimension 1 is special, see reference [14] for details
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13
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33644902214
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In a pure 2D system, there is only quasi-long-range order. We will however still use the terminology: CDW throughout the manuscript. As the system is strongly disordered there is no long-range order at all anyway (and it would be the same in the equivalent 3D geometry)
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In a pure 2D system, there is only quasi-long-range order. We will however still use the terminology: CDW throughout the manuscript. As the system is strongly disordered there is no long-range order at all anyway (and it would be the same in the equivalent 3D geometry)
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19
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33644918433
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edited by S. Brazovskii, N. Kirova, P. Monceau, J. Phys. IV France, (EDP Sciences)
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ECRYS-2005: International Workshop on Electronic Crystals, edited by S. Brazovskii, N. Kirova, P. Monceau, J. Phys. IV France, 131 (EDP Sciences, 2005)
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(2005)
ECRYS-2005: International Workshop on Electronic Crystals
, vol.131
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20
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33644919258
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It should be noticed that going beyond the Mott or ES arguments or proving from microscopics the VRH laws are still open and challenging problems. However, progress has been made towards deriving the Coulomb gap shape, see reference [20]
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It should be noticed that going beyond the Mott or ES arguments or proving from microscopics the VRH laws are still open and challenging problems. However, progress has been made towards deriving the Coulomb gap shape, see reference [20].
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22
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33644888414
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note
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el, up to a numerical factor
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23
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0001110704
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J. Joo, S.M. Long, J.P. Pouget, E.J. Oh, A.G. MacDiarmid, A.J. Epstein, Phys. Rev. B 57, 9567 (1998)
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(1998)
Phys. Rev. B
, vol.57
, pp. 9567
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Joo, J.1
Long, S.M.2
Pouget, J.P.3
Oh, E.J.4
MacDiarmid, A.G.5
Epstein, A.J.6
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26
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12044251389
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G. Blatter, M.V. Feigel'man, V.B. Geshkenbein, A.I. Larkin, V.M. Vinokur, Rev. Mod. Phys. 66, 1125 (1994)
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(1994)
Rev. Mod. Phys.
, vol.66
, pp. 1125
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Blatter, G.1
Feigel'man, M.V.2
Geshkenbein, V.B.3
Larkin, A.I.4
Vinokur, V.M.5
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28
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33644927927
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This follows from the fact that in quasi-1D systems, charges are constrained to move along lines, with a small hopping amplitude from one line to the other. For the Wigner crystal, where displacements are two-dimensional, the basic defect is the vacancy or the interstitial, with a length of the order of the distance between electrons
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This follows from the fact that in quasi-1D systems, charges are constrained to move along lines, with a small hopping amplitude from one line to the other. For the Wigner crystal, where displacements are two-dimensional, the basic defect is the vacancy or the interstitial, with a length of the order of the distance between electrons
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29
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0001889266
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edited by I.M. Khalatnikov (Harwood, New York)
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S. Brazovskii, N. Kirova, in Soviet Scientific Reviews, Sec. A, Physics Reviews, Vol. 6, edited by I.M. Khalatnikov (Harwood, New York, 1984)
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(1984)
Soviet Scientific Reviews, Sec. A, Physics Reviews
, vol.6
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Brazovskii, S.1
Kirova, N.2
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33644883777
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The f-scattering term is generally removed by a shift of the φ-field. One then works on the background of a deformed system. Here, we are interested in such deformations and we therefore consider explicitly the f-scattering term
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The f-scattering term is generally removed by a shift of the φ-field. One then works on the background of a deformed system. Here, we are interested in such deformations and we therefore consider explicitly the f-scattering term.
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