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1
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0001581456
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A. Schwartz, M. Dressel, G. Grüner, V. Vescoli, L. Degiorgi, and T. Giamarchi, Phys. Rev. B 58, 1261 (1998).
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(1998)
Phys. Rev. B
, vol.58
, pp. 1261
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Schwartz, A.1
Dressel, M.2
Grüner, G.3
Vescoli, V.4
Degiorgi, L.5
Giamarchi, T.6
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3
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85037895381
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Throughout this work we shall use units where (Formula presented) Although Eqs. (2) and (3) seem to fit the data rather well, one should keep in mind that the precise determination of the frequency dependence of the scattering rate is rather sensitive to the normalization and extrapolation of the data.
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Throughout this work we shall use units where (Formula presented) Although Eqs. (2) and (3) seem to fit the data rather well, one should keep in mind that the precise determination of the frequency dependence of the scattering rate is rather sensitive to the normalization and extrapolation of the data.
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4
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85037883055
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An upper limit for the crossover temperature is given by the hopping integral (Formula presented) between the chains: (Formula presented)
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An upper limit for the crossover temperature is given by the hopping integral (Formula presented) between the chains: (Formula presented)
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5
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0031634425
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J. Moser, M. Gabay, P. Auban-Senzier, D. Jérome, K. Bechgaard, and J. M. Fabre, Eur. Phys. J. B 1, 39 (1998).
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(1998)
Eur. Phys. J. B
, vol.1
, pp. 39
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Moser, J.1
Gabay, M.2
Auban-Senzier, P.3
Jérome, D.4
Bechgaard, K.5
Fabre, J.M.6
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7
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85037873736
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L. P. Gorkov, in Electron-Electron Interactions in Disordered Systems, edited by A. L. Efros and M. Pollak (North-Holland, Amsterdam, 1985). See the discussion on defects in quasi-one-dimensional conductors on p. 634.
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L. P. Gorkov, in Electron-Electron Interactions in Disordered Systems, edited by A. L. Efros and M. Pollak (North-Holland, Amsterdam, 1985). See the discussion on defects in quasi-one-dimensional conductors on p. 634.
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10
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85037893317
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T. Bohr, Nordita Report No. 1981 (unpublished).
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T. Bohr, Nordita Report No. 1981 (unpublished).
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19
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85037883704
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Note that Eqs. (15) and (16) are the leading behavior for small (Formula presented) so that it would be incorrect to perform a Kramers-Kronig analysis on these expressions. In contrast, the phenomenological Eqs. (2) and (3) interpolate from small to large frequencies.
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Note that Eqs. (15) and (16) are the leading behavior for small (Formula presented) so that it would be incorrect to perform a Kramers-Kronig analysis on these expressions. In contrast, the phenomenological Eqs. (2) and (3) interpolate from small to large frequencies.
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20
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85037882564
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Phys. Rev. B 59 (to be published).
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L. Bartosch and P. Kopietz, Phys. Rev. B 59 (to be published).
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Bartosch, L.1
Kopietz, P.2
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21
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12044251254
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D. Jérome, Science 252, 1509 (1991).
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(1991)
Science
, vol.252
, pp. 1509
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Jérome, D.1
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23
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85037915515
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We would like to thank George Grüner for pointing this out to us.
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We would like to thank George Grüner for pointing this out to us.
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