Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Entanglement Entropy and Entanglement Growth in Gauge Theory

Naoki Watamura, 尚毅 綿村

Published Mar 26, 2018• 0 citations
OpenAlex

Related papers

Entanglement entropy in gauge theories and the holographic principle for electric strings

P. V. Buividovich, M. I. Polikarpov

arXiv:0806.3376•Physics Letters B•Oct 29, 2008•215 citations

Entanglement entropy, dualities, and deconfinement in gauge theories

Anber, Mohamed M., Kolligs, Benjamin J.

•Aug 28, 2018•0 citations

Hilbert space fragmentation at the origin of disorder-free localization in the lattice Schwinger model

Jared Jeyaretnam, Tanmay Bhore, Jesse J. Osborne +2 more

Lattice gauge theories, the discrete counterparts of continuum gauge theories, provide a rich framework for studying non-equilibrium quantum dynamics. Recent studies suggest disorder-free localization in the lattice Schwinger model, but its origin remains unclear. Using a combination of analytical and numerical methods, we show that Hilbert space fragmentation emerges in the strong coupling limit, constraining particle dynamics and causing sharp jumps in entanglement entropy growth within charge sectors. By analyzing jump statistics, we find that entanglement growth follows a single-logarithmic or weak power-law dependence on time, rather than a double-logarithmic form. This suggests a single ergodicity-breaking regime that mimics many-body localization in finite systems due to fragmentation effects. Our findings clarify the nature of disorder-free localization and its distinction from conventional many-body localization, highlighting how gauge constraints influence thermalization in lattice gauge theories.

arXiv:2409.08320•Communications Physics•Apr 18, 2025•10 citations

On the definition of entanglement entropy in lattice gauge theories

Sinya Aoki A, Takumi Iritani, Masahiro Nozaki A +3 more

We focus on the issue of proper definition of entanglement entropy in lattice gauge theories, and examine a naive definition where gauge invariant states are viewed as elements of an extended Hilbert space which contains gauge non-invariant states as well. Working in the extended Hilbert space, we can define entanglement entropy associated with an arbitrary subset of links, not only for abelian but also for non-abelian theories. We then derive the associated replica formula. We also discuss the issue of gauge invariance of the entanglement entropy. In the Z N gauge theories in arbitrary space dimensions, we show that all the standard properties of the entanglement entropy, e.g. the strong subadditivity, hold in our definition. We study the entanglement entropy for special states, including the topological states for the Z N gauge theories in arbitrary dimensions. We discuss relations of our definition to other proposals.

arXiv:1502.04267•Journal of High Energy Physics•Jun 1, 2015•92 citations

Entanglement and thermal entropy of gauge fields

Christopher Eling, Yaron Oz, Stefan Theisen

arXiv:1308.4964•Journal of High Energy Physics•Nov 1, 2013•27 citations

Entanglement entropy in d+1 SU(N) gauge theory

Alexander Velytsky

We consider the entanglement entropy for a subsystem in $d+1$ dimensional $SU(N)$ lattice gauge theory. The $1+1$ gauge theory is treated exactly and shows trivial behavior. Gauge theories in higher dimensions are treated within Migdal-Kadanoff approximation. We consider the gauge theory in the confinement phase. We demonstrate the existence of a nonanalytical change from the short distance to long distance form in the entanglement entropy in such systems ($d>2$) reminiscent of phase transition. The transition is manifested in nontrivial change in the renormalization group flow of character expansion coefficients defining the partition function.

arXiv:0801.4111•Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields•Apr 24, 2008•39 citations
Lattice gauge theories, the discrete counterparts of continuum gauge theories, provide a rich framework for studying non-equilibrium quantum dynamics. Recent studies suggest disorder-free localization in the lattice Schwinger model, but its origin remains unclear. Using a combination of analytical and numerical methods, we show that Hilbert space fragmentation emerges in the strong coupling limit, constraining particle dynamics and causing sharp jumps in entanglement entropy growth within charge sectors. By analyzing jump statistics, we find that entanglement growth follows a single-logarithmic or weak power-law dependence on time, rather than a double-logarithmic form. This suggests a single ergodicity-breaking regime that mimics many-body localization in finite systems due to fragmentation effects. Our findings clarify the nature of disorder-free localization and its distinction from conventional many-body localization, highlighting how gauge constraints influence thermalization in lattice gauge theories.
We focus on the issue of proper definition of entanglement entropy in lattice gauge theories, and examine a naive definition where gauge invariant states are viewed as elements of an extended Hilbert space which contains gauge non-invariant states as well. Working in the extended Hilbert space, we can define entanglement entropy associated with an arbitrary subset of links, not only for abelian but also for non-abelian theories. We then derive the associated replica formula. We also discuss the issue of gauge invariance of the entanglement entropy. In the Z N gauge theories in arbitrary space dimensions, we show that all the standard properties of the entanglement entropy, e.g. the strong subadditivity, hold in our definition. We study the entanglement entropy for special states, including the topological states for the Z N gauge theories in arbitrary dimensions. We discuss relations of our definition to other proposals.
We consider the entanglement entropy for a subsystem in d+1d+1d+1 dimensional SU(N)SU(N)SU(N) lattice gauge theory. The 1+11+11+1 gauge theory is treated exactly and shows trivial behavior. Gauge theories in higher dimensions are treated within Migdal-Kadanoff approximation. We consider the gauge theory in the confinement phase. We demonstrate the existence of a nonanalytical change from the short distance to long distance form in the entanglement entropy in such systems (d>2d>2d>2) reminiscent of phase transition. The transition is manifested in nontrivial change in the renormalization group flow of character expansion coefficients defining the partition function.