Abstract

The pair localization length L2L_2 of two interacting electrons in one--dimensional disordered systems is studied numerically. Using two direct approaches, we find L2∝L1αL_2 \propto L_1^α, where L1L_1 is the one-electron localization length and α≈1.65α\approx 1.65. This demonstrates the enhancement effect proposed by Shepelyansky, but the value of αα differs from previous estimates (α=2α=2) in the disorder range considered. We explain this discrepancy using a scaling picture recently introduced by Imry and taking into account a more accurate distribution than previously assumed for the overlap of one-electron wavefunctions.

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