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arXiv:1808.09906 · Physical review. B./Physical review. B

Environment-induced prerelaxation in the Mott-Hubbard model

Friedemann Queißer, Ralf Schützhold

Published Apr 3, 2019• 13 citations
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Abstract

Via the hierarchy of correlations, we study the strongly interacting Fermi-Hubbard model in the Mott insulator state and couple it to a Markovian environment that constantly monitors the particle numbers ${\stackrel{\ifmmode \hat{}\else \^{}\fi{}}{n}}_{\ensuremath{\mu}}^{\ensuremath{\uparrow}}$ and ${\stackrel{\ifmmode \hat{}\else \^{}\fi{}}{n}}_{\ensuremath{\mu}}^{\ensuremath{\downarrow}}$ for each lattice site $\ensuremath{\mu}$. As expected, the environment induces an imaginary part $\ensuremath{\gamma}$ (i.e., the decay rate) of the quasiparticle frequencies ${\ensuremath{\omega}}_{\mathbf{k}}\ensuremath{\rightarrow}{\ensuremath{\omega}}_{\mathbf{k}}\ensuremath{-}i\ensuremath{\gamma}$, and it tends to diminish the correlations between lattice sites. Surprisingly, the environment also steers the state of the system on intermediate timescales $O(1/\ensuremath{\gamma})$ to a prerelaxed state very similar to the prethermalized state after a quantum quench (i.e., suddenly switching on the hopping rate $J$). Full relaxation or thermalization occurs via local on-site heating and takes much longer.

DOI
10.1103/physrevb.99.155110

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Via the hierarchy of correlations, we study the strongly interacting Fermi-Hubbard model in the Mott insulator state and couple it to a Markovian environment that constantly monitors the particle numbers n\ifmmode^\elseˆ\fi\ensuremathμ\ensuremath↑{\stackrel{\ifmmode \hat{}\else \^{}\fi{}}{n}}_{\ensuremath{\mu}}^{\ensuremath{\uparrow}}n\ifmmode^\elseˆ\fi\ensuremathμ\ensuremath↑​ and n\ifmmode^\elseˆ\fi\ensuremathμ\ensuremath↓{\stackrel{\ifmmode \hat{}\else \^{}\fi{}}{n}}_{\ensuremath{\mu}}^{\ensuremath{\downarrow}}n\ifmmode^\elseˆ\fi\ensuremathμ\ensuremath↓​ for each lattice site \ensuremathμ\ensuremath{\mu}\ensuremathμ. As expected, the environment induces an imaginary part \ensuremathγ\ensuremath{\gamma}\ensuremathγ (i.e., the decay rate) of the quasiparticle frequencies \ensuremathωk\ensuremath→\ensuremathωk\ensuremath−i\ensuremathγ{\ensuremath{\omega}}_{\mathbf{k}}\ensuremath{\rightarrow}{\ensuremath{\omega}}_{\mathbf{k}}\ensuremath{-}i\ensuremath{\gamma}\ensuremathωk​\ensuremath→\ensuremathωk​\ensuremath−i\ensuremathγ, and it tends to diminish the correlations between lattice sites. Surprisingly, the environment also steers the state of the system on intermediate timescales O(1/\ensuremathγ)O(1/\ensuremath{\gamma})O(1/\ensuremathγ) to a prerelaxed state very similar to the prethermalized state after a quantum quench (i.e., suddenly switching on the hopping rate JJJ). Full relaxation or thermalization occurs via local on-site heating and takes much longer.
For the Fermi-Hubbard model in the strongly interacting Mott insulator state, we study the prethermalization dynamics after a quench (switching on the hopping rate). To this end, we employ the method of the hierarchy of correlations and compare different levels of accuracy. To leading order, the usual free quasiparticle dynamics (as encoded in the two-point correlation functions) yields the standard picture of prethermalization. Taking into account the back-reaction of these quasiparticle fluctuations onto the mean-field background as the first next-to-leading-order effect, we observe a strong degradation of prethermalization, especially in low dimensions. In contrast, the inclusion of three-point correlations enhances prethermalization.
We study the dissipative Fermi-Hubbard model in the limit of weak tunneling and strong repulsive interactions, where each lattice site is tunnel-coupled to a Markovian fermionic bath. For cold baths at intermediate chemical potentials, the Mott insulator property remains stable and we find a fast relaxation of the particle number towards half filling. On longer time scales, we find that the antiferromagnetic order of the Mott-N\'eel ground state on bipartite lattices decays, even at zero temperature. For zero and nonzero temperatures, we quantify the different relaxation time scales by means of waiting time distributions, which can be derived from an effective (non-Hermitian) Hamiltonian and obtain fully analytic expressions for the Fermi-Hubbard model on a tetramer ring.
We study the Bose and Fermi Hubbard model in the (formal) limit of large coordination numbers Z≫1Z\gg1Z≫1. Via an expansion into powers of 1/Z1/Z1/Z, we establish a hierarchy of correlations which facilitates an approximate analytical derivation of the time-evolution of the reduced density matrices for one and two sites etc. With this method, we study the quantum dynamics (starting in the ground state) after a quantum quench, i.e., after suddenly switching the tunneling rate JJJ from zero to a finite value, which is still in the Mott regime. We find that the reduced density matrices approach a (quasi) equilibrium state after some time. For one lattice site, this state can be described by a thermal state (within the accuracy of our approximation). However, the (quasi) equilibrium state of the reduced density matrices for two sites including the correlations cannot be described by a thermal state. Thus, real thermalization (if it occurs) should take much longer time. This behavior has already been observed in other scenarios and is sometimes called ``pre-thermalization.'' Finally, we compare our results to numerical simulations for finite lattices in one and two dimensions and find qualitative agreement.
We study the Bose-Hubbard and Fermi-Hubbard models in the (formal) limit of large coordination numbers $Z\ensuremath{\gg}1$. Via an expansion into powers of 1/Z1/Z1/Z, we establish a hierarchy of correlations which facilitates an approximate analytical derivation of the time evolution of the reduced density matrices for one and two sites, etc. With this method, we study the quantum dynamics (starting in the ground state) after a quantum quench, i.e., after suddenly switching the tunneling rate JJJ from zero to a finite value, which is still in the Mott regime. We find that the reduced density matrices approach a (quasi)equilibrium state after some time. For one lattice site, this state can be described by a thermal state (within the accuracy of our approximation). However, the (quasi)equilibrium state of the reduced density matrices for two sites including the correlations can not be described by a thermal state. Thus, real thermalization (if it occurs) should take a much longer time. This behavior has already been observed in other scenarios and is sometimes called ``prethermalization''. Finally, we compare our results to numerical simulations for finite lattices in one and two dimensions and find qualitative agreement.
We study the Bose-Hubbard and Fermi-Hubbard model in the limit of large coordination numbers Z (i.e., many tunnelling partners). Via a controlled expansion into powers of 1/Z, we establish a hierarchy of correlations, which facilitates an approximate analytic solution of the quantum evolution. For the Bose-Hubbard model, we derive the growth of phase coherence after a quench from the Mott to the superfluid phase. For a quench within the Mott phase, we find that various local observables approach a quasi-equilibrium state after a finite period of time. However, this state is not thermal, i.e., real thermalisation -- if it occurs -- requires much longer time scales. For a tilted lattice in the Mott state, we calculate the tunnelling probability and find a remarkable analogy to the Sauter-Schwinger effect (i.e., electron-positron pair creation out of the vacuum due to a strong electric field). These analytical results are compared to numerical simulations for finite lattices in one and two dimensions and we find qualitative agreement. Finally, we generalize these studies to the more involved case of the Fermi-Hubbard model.
Via the hierarchy of correlations, we study the Mott insulator phase of the Fermi-Hubbard model in the limit of strong interactions and derive a quantum Boltzmann equation describing its relaxation dynamics. In stark contrast to the weakly interacting case, we find that the scattering cross sections strongly depend on the momenta of the colliding quasiparticles and holes. Therefore, the relaxation towards equilibrium crucially depends on the spectrum of excitations. For example, for particle-hole excitations directly at the minimum of the (direct) Mott gap, the scattering cross sections vanish such that these excitations can have a very long lifetime.