Scale-invariant phase transition of disordered bosons in one dimension

Fuente: arXiv
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Hauptverfasser: Gupta, Tanul, Masella, Guido, Mattiotti, Francesco, Prokof'ev, Nikolay V., Pupillo, Guido
Format: Preprint
Veröffentlicht: 2023
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author Gupta, Tanul
Masella, Guido
Mattiotti, Francesco
Prokof'ev, Nikolay V.
Pupillo, Guido
author_facet Gupta, Tanul
Masella, Guido
Mattiotti, Francesco
Prokof'ev, Nikolay V.
Pupillo, Guido
contents The disorder-induced quantum phase transition between superfluid and non-superfluid states of bosonic particles in one dimension is generally expected to be of the Berezinskii-Kosterlitz-Thouless (BKT) type. Here, we show that hard-core lattice bosons with integrable power-law hopping decaying with distance as $1/r^α$ - corresponding in spin language to a $XY$ model with power-law couplings - undergo a non-BKT continuous phase transition instead. We use exact quantum Monte-Carlo methods to determine the phase diagram for different values of the exponent $α$, focusing on the regime $α> 2$. We find that the scaling of the superfluid stiffness with the system size is scale-invariant at the transition point for any $α\leq 3$ - a behavior incompatible with the BKT scenario and typical of continuous phase transitions in higher dimension. By scaling analysis near the transition point, we find that our data are consistent with a correlation length exponent satisfying the Harris bound $ν\geq 2$ and demonstrate a new universal behavior of disordered bosons in one dimension. For $α>3$ our data are consistent with a BKT scenario where the liquid is pinned by infinitesimal disorder.
format Preprint
id arxiv_https___arxiv_org_abs_2310_17682
institution arXiv
publishDate 2023
record_format arxiv
spellingShingle Scale-invariant phase transition of disordered bosons in one dimension
Gupta, Tanul
Masella, Guido
Mattiotti, Francesco
Prokof'ev, Nikolay V.
Pupillo, Guido
Quantum Gases
Disordered Systems and Neural Networks
Quantum Physics
The disorder-induced quantum phase transition between superfluid and non-superfluid states of bosonic particles in one dimension is generally expected to be of the Berezinskii-Kosterlitz-Thouless (BKT) type. Here, we show that hard-core lattice bosons with integrable power-law hopping decaying with distance as $1/r^α$ - corresponding in spin language to a $XY$ model with power-law couplings - undergo a non-BKT continuous phase transition instead. We use exact quantum Monte-Carlo methods to determine the phase diagram for different values of the exponent $α$, focusing on the regime $α> 2$. We find that the scaling of the superfluid stiffness with the system size is scale-invariant at the transition point for any $α\leq 3$ - a behavior incompatible with the BKT scenario and typical of continuous phase transitions in higher dimension. By scaling analysis near the transition point, we find that our data are consistent with a correlation length exponent satisfying the Harris bound $ν\geq 2$ and demonstrate a new universal behavior of disordered bosons in one dimension. For $α>3$ our data are consistent with a BKT scenario where the liquid is pinned by infinitesimal disorder.
title Scale-invariant phase transition of disordered bosons in one dimension
topic Quantum Gases
Disordered Systems and Neural Networks
Quantum Physics
url https://arxiv.org/abs/2310.17682