Many-body localisation is a fascinating
example of a scenario in which interacting quantum systems isolated from
their environments can fail to thermalise. Key to our understanding of
this enigmatic phase of matter are emergent conserved quantities known
as local integrals of motion (LIOMs, or l-bits), which prevent
thermalisation from occurring. In this talk, I will present a powerful
new numerical method known as the ‘tensor flow equation’ technique
ideally suited for computing LIOMs [1]. Using this method, we’ll look at
a model of interacting fermions in a quasiperiodic potential and show
that an MBL phase exists. We will directly compute the LIOMs and show
how – in contrast to disordered systems – they retain a strong
fingerprint of the underlying quasiperiodic potential. Time permitting, I’ll also sketch how
this technique can be used to address non-equilibrium dynamics [2],
periodically driven systems [3], and dissipative dynamics [4], as well
as extensions to two [2] and even three dimensions.
[1] – S. J. Thomson and M. Schiró, https://arxiv.org/abs/2110.02906 [2] – S. J. Thomson and M. Schiró, Physical Review B 97 (6), 060201(R) and Physical Review Research 2 (4), 043368 [3] – S. J. Thomson, D. Magano and M. Schiró, SciPost Phys. 11 (028) [4] – L. Rosso et al., SciPost Phys. 9, 091