Decay of density waves in coupled one-dimensional many-body-localized systems

The behavior of coupled disordered one-dimensional systems, as modelled by identical fermionic Hubbard chains with the on-site potential disorder and coupling emerging through the inter-chain hopping $t'$, is analysed. The study is motivated by the experiment on fermionic cold atoms on a disordered lattice, where a decay rate of the quenched density wave was measured. We present a derivation of the decay rate $Γ$ within perturbation theory and show that even at large disorder along the chains the interaction leads to finite $Γ> 0$, the mechanism being the interaction-induced coupling of in-chain localized and inter-chain extended single-fermion states. Explicit expressions for $Γ$ are presented for a weak interaction $U < t,t'$, but extended also to the regime $t > U >t'$. It is shown that in both regimes $Γ$ increases with the inter-chain hopping $t'$, as well as decreases with increasing disorder.

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