Abstract
The effect of long-range electron-electron interactions on the existence of a mobility edge and on the characteristics of critical localization behaviour is studied for disordered systems by means of a 1/n-expansion in the finite temperature technique of many body theory. The lower critical dimension turns out to be two as in ensembles with interaction-free hamiltonians, and a subsequent d-2 expansion applies. In the case of time reversal invariance and in 0(1/n), cancellations of correlation contributions leave the conductivity behaviour unchanged when the Fermi energy approaches the still existing mobility edge(continuous transition). Many body effects however introduce criticality into one-particle properties and the density of states p(EF) vanishes with the critical exponent β-1/(d-2)+0((d-2)°) when EF-Ec goes to zero on the metallic side f the transition. In the case of broken time reversal invariance the 0(1/n) approximation gives rise to speculations on a first order transition, but 0(1/n2) calculations are indispensable for a reliable conclusion.
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© 1981 Springer-Verlag
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Oppermann, R. (1981). On effects of electron-electron interactions in disordered electronic systems. In: Castellani, C., Di Castro, C., Peliti, L. (eds) Disordered Systems and Localization. Lecture Notes in Physics, vol 149. Springer, Berlin, Heidelberg. https://doi.org/10.1007/BFb0012564
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DOI: https://doi.org/10.1007/BFb0012564
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