Transport on the ergodic side of the many-body localisation transition in the absence of conserved quantities
We consider the question of what happens to sub diffusion in periodically driven Floquet many-body localized systems when there are no conserved quantities. We develop a numerical technique that allows us to reliably study relatively large system sizes and large times. We observe what looks like stretched exponential dependence of correlation functions, but with some flow of exponent with system size.