Stationary time correlations for fermions after a quench in the presence of an impurity
arXiv:2211.15447 · doi:10.1209/0295-5075/accec7
Abstract
We consider the quench dynamics of non-interacting fermions in one dimension in the presence of a finite-size impurity at the origin. This impurity is characterized by general momentum-dependent reflection and transmission coefficients which are changed from to at time . The initial state is at equilibrium with such that the system is cut in two independent halves with , respectively to the right and to the left of the impurity. We obtain the exact large time limit of the multi-time correlations. These correlations become time translationally invariant, and are non-zero in two different regimes: (i) for where the system reaches a non-equilibrium steady state (NESS) (ii) for , i.e., the ray-regime. For a repulsive impurity these correlations are independent of , , while in the presence of bound states they oscillate and memory effects persist. We show that these nontrivial relaxational properties can be retrieved in a simple manner from the large time behaviour of the single particle wave functions.
arXiv commentMain text: 7 pages, 3 figures. Supp. Mat.: 31 pages, 4 figures
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