Disorder-Free Localization
ORAL
Abstract
The venerable phenomena of Anderson localization, along with the much more recent many-body localization, both depend crucially on the presence of disorder. The latter enters either in the form of quenched disorder in the parameters of the Hamiltonian, or through a special choice of a disordered initial state. Here, we present a family of very simple translationally invariant quantum models with only local interactions between spins and fermions. By identifying an extensive set of conserved quantities, we show that the system generates purely dynamically its own disorder, which gives rise to localization of fermionic degrees of freedom. Our work provides an answer to a decades old question whether quenched disorder is a necessary condition for localization. It also offers new insights into the physics of many-body localization, lattice gauge theories, and quantum disentangled liquids.
References:
Phys. Rev. Lett. 118, 266601 (2017),
Phys. Rev. Lett. 119, 176601 (2017)
References:
Phys. Rev. Lett. 118, 266601 (2017),
Phys. Rev. Lett. 119, 176601 (2017)
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Presenters
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Adam Smith
Theory of Condensed Matter Group, University of Cambridge
Authors
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Adam Smith
Theory of Condensed Matter Group, University of Cambridge
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Johannes Knolle
Theory of Condensed Matter Group, University of Cambridge
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Roderich Moessner
Max Planck Institute for the Physics of Complex Systems, Max Planck Institut für Physik komplexer Systeme, Max-Planck-Institute for the Physics of Complex Systems (MPI-PKS), MPIPKS, Max Planck Inst, Max-Planck-Institute for the Physics of Complex Systems
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Dmitry Kovrizhin
Rudolf Peierls Centre for Theoretical Physics, University of Oxford