Many-body localization and enhanced non-ergodic sub-diffusive regime in
the presence of random long-range interactions
- URL: http://arxiv.org/abs/2010.12485v3
- Date: Mon, 8 Feb 2021 16:28:00 GMT
- Title: Many-body localization and enhanced non-ergodic sub-diffusive regime in
the presence of random long-range interactions
- Authors: Yogeshwar Prasad and Arti Garg
- Abstract summary: We study many-body localization (MBL) in a one-dimensional system of spinless fermions with a deterministic aperiodic potential.
We demonstrate that MBL survives even for $alpha 1$ and is preceded by a broad non-ergodic sub-diffusive phase.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: We study many-body localization (MBL) in a one-dimensional system of spinless
fermions with a deterministic aperiodic potential in the presence of long-range
interactions decaying as power-law $V_{ij}/(r_i-r_j)^\alpha$ with distance and
having random coefficients $V_{ij}$. We demonstrate that MBL survives even for
$\alpha <1$ and is preceded by a broad non-ergodic sub-diffusive phase.
Starting from parameters at which the short-range interacting system shows
infinite temperature MBL phase, turning on random power-law interactions
results in many-body mobility edges in the spectrum with a larger fraction of
ergodic delocalized states for smaller values of $\alpha$. Hence, the critical
disorder $h_c^r$, at which ergodic to non-ergodic transition takes place
increases with the range of interactions. Time evolution of the density
imbalance $I(t)$, which has power-law decay $I(t) \sim t^{-\gamma}$ in the
intermediate to large time regime, shows that the critical disorder $h_{c}^I$,
above which the system becomes diffusion-less (with $\gamma \sim 0$) and
transits into the MBL phase is much larger than $h_c^r$. In between $h_{c}^r$
and $h_{c}^I$ there is a broad non-ergodic sub-diffusive phase, which is
characterized by the Poissonian statistics for the level spacing ratio,
multifractal eigenfunctions and a non zero dynamical exponent $\gamma \ll 1/2$.
The system continues to be sub-diffusive even on the ergodic side ($h < h_c^r$)
of the MBL transition, where the eigenstates near the mobility edges are
multifractal. For $h < h_{0}<h_c^r$, the system is super-diffusive with $\gamma
>1/2$. The rich phase diagram obtained here is unique to random nature of
long-range interactions. We explain this in terms of the enhanced correlations
among local energies of the effective Anderson model induced by random
power-law interactions.
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