Measurement-induced phase transition in a single-body tight-binding model

We study the statistical properties of a single free quantum particle evolving coherently on a discrete lattice in $\mathit{\text{d}}$ spatial dimensions where every lattice site is additionally subject to continuous measurement of the occupation number. Our numerical results indicate that the system undergoes a measurement-induced phase transition (MiPT) for $\mathit{\text{d}}>1$ from a delocalized to a localized phase as the measurement strength $\ensuremath{\gamma}$ is increased beyond a critical value ${\ensuremath{\gamma}}_{c}$. In the language of surface growth, the delocalized phase corresponds to a smooth phase while the localized phase corresponds to a rough phase. We support our numerical results with perturbative renormalization group (RG) computations which are in qualitative agreement at one-loop order.

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Publication Details

Journal
Physical review. B./Physical review. B
Published
2024-08-19
DOI
https://doi.org/10.1103/physrevb.110.l060202
Citations
16
Primary Topic
Quantum many-body systems
Type
article
Field-Weighted Citation Impact
5.40
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article

Measurement-induced phase transition in a single-body tight-binding model

Tony Jin, D.G. Martin
16 citations
Physical review. B./Physical review. B
Quantum many-body systems
5.40
article

Measurement-induced phase transition in a single-body tight-binding model

Tony Jin, D.G. Martin
article en
16 citations

Abstract

We study the statistical properties of a single free quantum particle evolving coherently on a discrete lattice in $\mathit{\text{d}}$ spatial dimensions where every lattice site is additionally subject to continuous measurement of the occupation number. Our numerical results indicate that the system undergoes a measurement-induced phase transition (MiPT) for $\mathit{\text{d}}>1$ from a delocalized to a localized phase as the measurement strength $\ensuremath{\gamma}$ is increased beyond a critical value ${\ensuremath{\gamma}}_{c}$. In the language of surface growth, the delocalized phase corresponds to a smooth phase while the localized phase corresponds to a rough phase. We support our numerical results with perturbative renormalization group (RG) computations which are in qualitative agreement at one-loop order.

Physical review. B./Physical review. BVol. 110(6)
Université Côte d'Azur (FR), University of Chicago (US), Observatoire de la Côte d’Azur (FR), Institut de Physique de Nice (FR)
Climate action
Openalex Percentile: Top 3%
Quantum many-body systems
5.40
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