Charge and spin-specific local integrals of motion in a disordered Hubbard model
arXiv:1903.01049 · doi:10.1103/PhysRevB.100.125132
Abstract
While many-body localization has primarily been studied in systems with a single local degree of freedom, experimental studies of many-body localization in cold atom systems motivate exploration of the disordered Hubbard model. With two coupled local degrees of freedom it is natural to ask how localization in spin relates to disorder in charge and vice versa. Most prior work has addressed disorder in only one of these sectors and often has not used measures of localization which distinguish between charge and spin. Here we explore localization in the Hubbard model with a wide range of independent values of charge and spin disorder, using measures of localization based on charge and spin-specific integrals of motion. Our results demonstrate symmetry between the response of the spin to charge disorder and vice versa, and we find very weak disorder in one channel, so long as the disorder in the other channel is sufficiently strong, results in localization in both channels. The strength of disorder required in the less disordered channel declines as the system size increases. Further, the weaker the disorder in the less-disordered channel, the longer the time scale at which localization appears in the dynamics of this degree of freedom.
7 pages, 5 figures, includes new data on larger systems
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- Many-body localization with synthetic gauge fields in disordered Hubbard chains
- Phenomenology of many-body localization in bond-disordered spin chains
- Many-body localization of 1D disordered impenetrable two-component fermions
- Disorder-induced spin-charge separation in the 1-D Hubbard model
- Contour-time approach to the disordered Bose-Hubbard model in the strong coupling regime
- Disordered impenetrable two-component fermions in one dimension