Mott transition for a Lieb-Liniger gas in a shallow quasiperiodic potential: Delocalization induced by disorder

Fuente: arXiv
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Main Authors: Yao, Hepeng, Tanzi, Luca, Sanchez-Palencia, Laurent, Giamarchi, Thierry, Modugno, Giovanni, D'Errico, Chiara
Format: Preprint
Published: 2024
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_version_ 1866929599938560000
author Yao, Hepeng
Tanzi, Luca
Sanchez-Palencia, Laurent
Giamarchi, Thierry
Modugno, Giovanni
D'Errico, Chiara
author_facet Yao, Hepeng
Tanzi, Luca
Sanchez-Palencia, Laurent
Giamarchi, Thierry
Modugno, Giovanni
D'Errico, Chiara
contents Disorder or quasi-disorder is known to favor the localization in many-body Bose systems. Here in contrast, we demonstrate an anomalous delocalization effect induced by incommensurability in quasiperiodic lattices. Loading ultracold atoms in two shallow periodic lattices with equal amplitude and either equal or incommensurate spatial periods, we show the onset of a Mott transition not only in the periodic case but also in the quasiperiodic case. Upon increase of the incommensurate component of the potential we find that the Mott insulator turns into a delocalized superfluid. Our experimental results agree with quantum Monte Carlo calculations, showing anomalous delocalization induced by the interplay between the commensuration and interaction.
format Preprint
id arxiv_https___arxiv_org_abs_2402_15318
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Mott transition for a Lieb-Liniger gas in a shallow quasiperiodic potential: Delocalization induced by disorder
Yao, Hepeng
Tanzi, Luca
Sanchez-Palencia, Laurent
Giamarchi, Thierry
Modugno, Giovanni
D'Errico, Chiara
Quantum Gases
Disordered Systems and Neural Networks
Disorder or quasi-disorder is known to favor the localization in many-body Bose systems. Here in contrast, we demonstrate an anomalous delocalization effect induced by incommensurability in quasiperiodic lattices. Loading ultracold atoms in two shallow periodic lattices with equal amplitude and either equal or incommensurate spatial periods, we show the onset of a Mott transition not only in the periodic case but also in the quasiperiodic case. Upon increase of the incommensurate component of the potential we find that the Mott insulator turns into a delocalized superfluid. Our experimental results agree with quantum Monte Carlo calculations, showing anomalous delocalization induced by the interplay between the commensuration and interaction.
title Mott transition for a Lieb-Liniger gas in a shallow quasiperiodic potential: Delocalization induced by disorder
topic Quantum Gases
Disordered Systems and Neural Networks
url https://arxiv.org/abs/2402.15318