We present an effective elastic theory which {\em quantitatively} describes the stripe phase of the two-dimensional electron gas in high Landau levels (N≥2). The dynamical matrix is obtained with remarkably high precision from the density-density correlation function in the time-dependent Hartree-Fock approximation. A renormalization group analysis shows that at T=0, as the partial filling factor Δν≡ν−⌊ν⌋ moves away from 1/2, the anisotropic conducting state may undergo quantum phase transitions: stripes may get pinned along their conducting direction by disorder, or may lock into one another to form a two-dimensional crystal. The model predicts values of Δν for each transition. The transitions should be reflected in the temperature dependence of the dissipative conductivity.
@article{arxiv.cond-mat/0003139,
title = {Stability of the Smectic Quantum Hall State: A Quantitative Study},
author = {Hangmo Yi and H. A. Fertig and R. Cote},
journal= {arXiv preprint arXiv:cond-mat/0003139},
year = {2009}
}