Abstract
We obtain exact analytical results for the evolution of a 1+1-dimensional Luttinger model prepared in a domain wall initial state, i.e., a state with different densities on its left and right sides. Such an initial state is modeled as the ground state of a translation invariant Luttinger Hamiltonian \({H_{\lambda}}\) with short range non-local interaction and different chemical potentials to the left and right of the origin. The system evolves for time t > 0 via a Hamiltonian \({H_{\lambda'}}\) which differs from \({H_{\lambda}}\) by the strength of the interaction. Asymptotically in time, as \({t \to \infty}\), after taking the thermodynamic limit, the system approaches a translation invariant steady state. This final steady state carries a current I and has an effective chemical potential difference \({\mu_{+} - \mu_{-}}\) between right- (+) and left- (−) moving fermions obtained from the two-point correlation function. Both I and \({\mu_{+} - \mu_{-}}\) depend on \({\lambda}\) and \({\lambda'}\). Only for the case \({\lambda = \lambda' = 0}\) does \({\mu_{+} - \mu_{-}}\) equal the difference in the initial left and right chemical potentials. Nevertheless, the Landauer conductance for the final state, \({G = I/(\mu_{+} - \mu_{-})}\), has a universal value equal to the conductance quantum \({e^2/h}\) for the spinless case.
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Langmann, E., Lebowitz, J.L., Mastropietro, V. et al. Steady States and Universal Conductance in a Quenched Luttinger Model. Commun. Math. Phys. 349, 551–582 (2017). https://doi.org/10.1007/s00220-016-2631-x
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DOI: https://doi.org/10.1007/s00220-016-2631-x