Numéro |
J. Phys. I France
Volume 3, Numéro 1, January 1993
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Page(s) | 143 - 169 | |
DOI | https://doi.org/10.1051/jp1:1993122 |
J. Phys. I France 3 (1993) 143-169
Nuclear relaxation and electronic correlations in quasi-one-dimensional organic conductors. I. Scaling theory
C. BourbonnaisCentre de Recherche en Physique du Solide, Département de Physique, Université de Sherbrooke, Sherbrooke, Québec, Canada, J1K-2R1 and Laboratoire de Physique des Solides, Université de Paris-Sud, Bât. 510, 91405 Orsay Cedex, France
(Received 21 April 1992, accepted in final form 4 September 1992)
Abstract
In this paper the results of the scaling theory for the quasi-one-dimensional electron gas model are used to make a detailed
analysis of the temperature variation of the nuclear relaxation rate for quasi-one-dimensional conductors which present an
antiferromagnetic critical point. From the extended dynamic scaling hypothesis, we show how the statics, the dynamics and
the dimensionality of antiferromagnetic and uniform spin fluctuations are involved in the power law behaviours of
for both the normal and the critical temperature domains. The full expressions of the antiferromagnetic contribution to
, the related critical indices as well as the dimensionality crossover scaling functions are derived in the cases where either
the interchain exchange or the quasi-1D nesting of the Fermi surface drives the transition. As for the influence of uniform
spin fluctuations, a derivation for the temperature dependent enhancement of the magnetic susceptibility
in one dimension is given. It is found that the harmonic character of collisionless paramagnons yields to the following scaling
law
which dominates at high temperature with an indice that depends on the dimensionality
D of the system. All the direct calculations are shown to be consistent with the scaling hypothesis.
76.60E - 74.70K - 75.40E - 75.50E
© Les Editions de Physique 1993