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19 April 2024
 
  » arxiv » cond-mat/9311018

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Fermi Edge Singularities and Backscattering in a Weakly Interacting 1D Electron Gas
C. L. Kane ; K. A. Matveev ; L. I. Glazman ;
Date 9 Nov 1993
Subject cond-mat
AbstractThe photon-absorption edge in a weakly interacting one-dimensional electron gas is studied, treating backscattering of conduction electrons from the core hole exactly. Close to threshold, there is a power-law singularity in the absorption, $I(epsilon) propto epsilon^{-alpha}$, with $alpha = 3/8 + delta_+/pi - delta_+^2/2pi^2$ where $delta_+$ is the forward scattering phase shift of the core hole. In contrast to previous theories, $alpha$ is finite (and universal) in the limit of weak core hole potential. In the case of weak backscattering $U(2k_F)$, the exponent in the power-law dependence of absorption on energy crosses over to a value $alpha = delta_+/pi - delta_+^2/2pi^2$ above an energy scale $epsilon^* sim [U(2k_F)]^{1/gamma}$, where $gamma$ is a dimensionless measure of the electron-electron interactions.
Source arXiv, cond-mat/9311018
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