4.6 Article

Avalanches and many-body resonances in many-body localized systems

Journal

PHYSICAL REVIEW B
Volume 105, Issue 17, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.105.174205

Keywords

-

Funding

  1. DARPA DRINQS program
  2. Sloan Foundation
  3. U.S. Department of Energy, Office of Science, Basic Energy Sciences [DE-SC0021111]
  4. Deutsche Forschungsgemeinschaft through SFB 1143 [247310070]
  5. Deutsche Forschungsgemeinschaft through the cluster of excellence ML4Q (EXC2004) [390534769]
  6. U.S. Department of Energy (DOE) [DE-SC0021111] Funding Source: U.S. Department of Energy (DOE)

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In this study, we numerically investigate the avalanche instability and many-body resonances in strongly disordered spin chains exhibiting many-body localization (MBL). We find that finite-size systems behave like MBL within the MBL regimes, and we identify landmarks that divide the MBL regimes into different subregimes based on the onset of avalanches and many-body resonances.
We numerically study both the avalanche instability and many-body resonances in strongly disordered spin chains exhibiting many-body localization (MBL). Finite-size systems behave like MBL within the MBL regimes, which we divide into the asymptotic MBL phase and the finite-size MBL regime; the latter regime is, however, thermal in the limit of large systems and long times. In both Floquet and Hamiltonian models, we identify some landmarks within the MBL regimes. Our first landmark is an estimate of where the MBL phase becomes unstable to avalanches, obtained by measuring the slowest relaxation rate of a finite chain coupled to an infinite bath at one end. Our estimates indicate that the actual MBL-to-thermal phase transition occurs much deeper in the MBL regimes than has been suggested by most previous studies. Our other landmarks involve systemwide many-body resonances: We find that the effective matrix elements producing eigenstates with systemwide many-body resonances are enormously broadly distributed. This broad distribution means that the onset of such resonances in typical samples occurs quite deep in the MBL regimes, and the first such resonances typically involve rare pairs of eigenstates that are farther apart in energy than the minimum gap. Thus we find that the resonance properties define two landmarks that divide the MBL regimes of finite-size systems into three subregimes: (i) at strongest randomness, typical samples do not have any eigenstates that are involved in systemwide many-body resonances; (ii) there is a substantial intermediate subregime where typical samples do have such resonances but the pair of eigenstates with the minimum spectral gap does not, so the size of the minimum gap agrees with expectations from Poisson statistics; and (iii) in the weaker randomness subregime, the minimum gap is larger than predicted by Poisson level statistics because it is involved in a many-body resonance and thus subject to level repulsion. Nevertheless, even in this third subregime, all but a vanishing fraction of eigenstates remain nonresonant and the system thus still appears MBL in most respects. Based on our estimates of the location of the avalanche instability, it might be that the MBL phase is only part of subregime (i) and the other subregimes are entirely in the thermal phase, even though they look localized in most respects, so are in the finite-size MBL regime.

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