Deformation of localized states and state transitions in systems of randomly hopping interacting fermions
arXiv:2110.14410 · doi:10.1103/PhysRevB.105.094201
Abstract
We numerically study the random-hopping fermions (the Cruetz ladder) with repulsion and investigate how the interactions deform localized eigenstates by means of the one particle-density matrix (OPDM). The ground state exhibits resurgence of localization from the compact localized state to strong-repulsion-induced localization. On the other hand, excited states in the middle of the spectrum tend to extend by the repulsion. The transition property obtained by numerical calculations of the OPDM is deeply understood by studying a solvable model in which local integrals of motion (LIOMs) are obtained explicitly. The present work clarifies the utility of the OPDM and also how compact-support LIOMs in non-interacting limit are deformed by the repulsion.
8 pages, 8 figures
References in corpus (9)
- Many body localization and thermalization in quantum statistical mechanics
- Phenomenology of fully many-body-localized systems
- QuSpin: a Python Package for Dynamics and Exact Diagonalisation of Quantum Many Body Systems part I: spin chains
- Recent progress in many-body localization
- Topology induced anomalous defect production by crossing a quantum critical point
- Many-Body Flatband Localization
- Fock-space anatomy of eigenstates across the many-body localisation transition
- Interplay and competition between disorder and flat band in an interacting Creutz ladder
- Multifractality and Fock-space localization in many-body localized states: one-particle density matrix perspective
Cited by in corpus (4)
- Fermion production at the boundary of an expanding universe: a cold-atom gravitational analogue
- Quantum information spreading in random spin chains with topological order
- Disorder in interacting quasi-one-dimensional systems: flat and dispersive bands
- Interplay of many-body interactions and quasiperiodic disorder in the all-band-flat diamond chain