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

arXiv:1807.01800 · Physical review. B./Physical review. B

Towards a generalized hydrodynamics description of Rényi entropies in integrable systems

Vincenzo Alba

Published Jan 29, 2019• 52 citations
arXivHTMLPDF

Abstract

We investigate the steady-state R\'enyi entanglement entropies after a quench from a piecewise homogeneous initial state in integrable models. In the quench protocol, two macroscopically different chains (leads) are joined together at the initial time, and the subsequent dynamics is studied. We study the entropies of a finite subsystem at the interface between the two leads. The density of R\'enyi entropies coincides with that of the entropies of the generalized Gibbs ensemble that describes the interface between the chains. By combining the generalized hydrodynamics treatment of the quench with the Bethe ansatz approach for the R\'enyi entropies, we provide exact results for quenches from several initial states in the anisotropic Heisenberg chain (XXZ chain), although the approach is applicable, in principle, to any low-entangled initial state and any integrable model. An interesting protocol that we consider is the expansion quench, in which one of the two leads is prepared in the vacuum of the model excitations. An intriguing feature is that for moderately large anisotropy the transport of bound state is not allowed. Moreover, we show that there is a ``critical'' anisotropy, below which bound-state transport is permitted. This is reflected in the steady-state entropies, which for large enough anisotropy do not contain information about the bound states. Finally, we benchmark our results against time-dependent density matrix renormalization group simulations.

DOI
10.1103/physrevb.99.045150

Related papers

Rényi entropies after releasing the Néel state in the XXZ spin-chain

Vincenzo Alba, Pasquale Calabrese

Abstract We study the Rényi entropies in the spin- 1 / 2 anisotropic Heisenberg chain after a quantum quench starting from the Néel state. The quench action method allows us to obtain the stationary Rényi entropies for arbitrary values of the index α as generalised free energies evaluated over a calculable thermodynamic macrostate depending on α . We work out this macrostate for several values of α and of the anisotropy Δ by solving the thermodynamic Bethe ansatz equations. By varying α different regions of the Hamiltonian spectrum are accessed. The two extremes are α → ∞ for which the thermodynamic macrostate is either the ground state or a low-lying excited state (depending on Δ) and α = 0 when the macrostate is the infinite temperature state. The Rényi entropies are easily obtained from the macrostate as function of α and a few interesting limits are analytically characterised. We provide robust numerical evidence to confirm our results using exact diagonalisation and a stochastic numerical implementation of Bethe ansatz. Finally, using tDMRG we calculate the time evolution of the Rényi entanglement entropies. For large subsystems and for any α , their density turns out to be compatible with that of the thermodynamic Rényi entropies.

arXiv:1709.02193•Journal of Statistical Mechanics Theory and Experiment•Nov 1, 2017•77 citations

Rényi entropies of generic thermodynamic macrostates in integrable systems

Márton Mestyán, Vincenzo Alba, Pasquale Calabrese

We study the behaviour of Renyi entropies in a generic thermodynamic macrostate of an integrable model. In the standard quench action approach to quench dynamics, the Renyi entropies may be derived from the overlaps of the initial state with Bethe eigenstates. These overlaps fix the driving term in the thermodynamic Bethe ansatz (TBA) formalism. We show that this driving term can be also reconstructed starting from the macrostate's particle densities. We then compute explicitly the stationary Renyi entropies after the quench from the dimer and the tilted Neel state in XXZ spin chains. For the former state we employ the overlap TBA approach, while for the latter we reconstruct the driving terms from the macrostate. We discuss in full detail the limits that can be analytically handled and we use numerical simulations to check our results against the large time limit of the entanglement entropies.

•Jan 1, 2018•42 citations

Rényi entropies of generic thermodynamic macrostates in integrable systems

Márton Mestyán, Vincenzo Alba, Pasquale Calabrese

Abstract We study the behaviour of Rényi entropies in a generic thermodynamic macrostate of an integrable model. In the standard quench action approach to quench dynamics, the Rényi entropies may be derived from the overlaps of the initial state with Bethe eigenstates. These overlaps fix the driving term in the thermodynamic Bethe ansatz (TBA) formalism. We show that this driving term can be also reconstructed starting from the macrostate’s particle densities. We then compute explicitly the stationary Rényi entropies after the quench from the dimer and the tilted Néel state in XXZ spin chains. For the former state we employ the overlap TBA approach, while for the latter we reconstruct the driving terms from the macrostate. We discuss in full detail the limits that can be analytically handled and we use numerical simulations to check our results against the large time limit of the entanglement entropies.

arXiv:1806.00624•Journal of Statistical Mechanics Theory and Experiment•Aug 1, 2018•41 citations

Entanglement and quantum transport in integrable systems

Vincenzo Alba

Understanding the entanglement structure of out-of-equilibrium many-body systems is a challenging, yet revealing task. Here, the author investigates the entanglement dynamics after a quench from a piecewise homogeneous state. This is the prototypical setup for studying quantum transport. By using a generalized hydrodynamic approach for integrable models and the quasiparticle picture for the entanglement dynamics, he conjectures a formula for the entanglement production rate after joining two semi-infinite homogeneous states, as well as for the steady-state entanglement entropy of a finite region. Interestingly, both quantities are determined by the physics, describing the interface between the two reservoirs.

arXiv:1706.00020•Physical review. B./Physical review. B•Jun 22, 2018•106 citations

Magnetization and entanglement after a geometric quench in the XXZ chain

Matthias Gruber, Viktor Eisler

We investigate the dynamics of the XXZ spin chain after a geometric quench, which is realized by connecting two half chains prepared in their ground states with zero and maximum magnetizations, respectively. The profiles of magnetization after the subsequent time evolution are studied numerically by density-matrix renormalization group methods, and a comparison to the predictions of generalized hydrodynamics yields a very good agreement. We also calculate the profiles of entanglement entropy and propose an ansatz for the noninteracting XX case, based on arguments from conformal field theory. In the general interacting case, the propagation of the entropy front is studied numerically both before and after the reflection from the chain boundaries. Finally, our results for the magnetization fluctuations indicate a leading order proportionality relation to the entanglement entropy.

arXiv:1902.05834•Physical review. B./Physical review. B•May 6, 2019•34 citations

Entanglement dynamics after quantum quenches in generic integrable systems

Vincenzo Alba, Pasquale Calabrese

The time evolution of the entanglement entropy in non-equilibrium quantum systems provides crucial information about the structure of the time-dependent state. For quantum quench protocols, by combining a quasiparticle picture for the entanglement spreading with the exact knowledge of the stationary state provided by Bethe ansatz, it is possible to obtain an exact and analytic description of the evolution of the entanglement entropy. Here we discuss the application of these ideas to several integrable models. First we show that for non-interacting systems, both bosonic and fermionic, the exact time-dependence of the entanglement entropy can be derived by elementary techniques and without solving the dynamics. We then provide exact results for interacting spin chains that are carefully tested against numerical simulations. Finally, we apply this method to integrable one-dimensional Bose gases (Lieb-Liniger model) both in the attractive and repulsive regimes. We highlight a peculiar behaviour of the entanglement entropy due to the absence of a maximum velocity of excitations.

arXiv:1712.07529•SciPost Physics•Mar 27, 2018•307 citations
We investigate the steady-state R'enyi entanglement entropies after a quench from a piecewise homogeneous initial state in integrable models. In the quench protocol, two macroscopically different chains (leads) are joined together at the initial time, and the subsequent dynamics is studied. We study the entropies of a finite subsystem at the interface between the two leads. The density of R'enyi entropies coincides with that of the entropies of the generalized Gibbs ensemble that describes the interface between the chains. By combining the generalized hydrodynamics treatment of the quench with the Bethe ansatz approach for the R'enyi entropies, we provide exact results for quenches from several initial states in the anisotropic Heisenberg chain (XXZ chain), although the approach is applicable, in principle, to any low-entangled initial state and any integrable model. An interesting protocol that we consider is the expansion quench, in which one of the two leads is prepared in the vacuum of the model excitations. An intriguing feature is that for moderately large anisotropy the transport of bound state is not allowed. Moreover, we show that there is a ``critical'' anisotropy, below which bound-state transport is permitted. This is reflected in the steady-state entropies, which for large enough anisotropy do not contain information about the bound states. Finally, we benchmark our results against time-dependent density matrix renormalization group simulations.
Abstract We study the Rényi entropies in the spin- 1 / 2 anisotropic Heisenberg chain after a quantum quench starting from the Néel state. The quench action method allows us to obtain the stationary Rényi entropies for arbitrary values of the index α as generalised free energies evaluated over a calculable thermodynamic macrostate depending on α . We work out this macrostate for several values of α and of the anisotropy Δ by solving the thermodynamic Bethe ansatz equations. By varying α different regions of the Hamiltonian spectrum are accessed. The two extremes are α → ∞ for which the thermodynamic macrostate is either the ground state or a low-lying excited state (depending on Δ) and α = 0 when the macrostate is the infinite temperature state. The Rényi entropies are easily obtained from the macrostate as function of α and a few interesting limits are analytically characterised. We provide robust numerical evidence to confirm our results using exact diagonalisation and a stochastic numerical implementation of Bethe ansatz. Finally, using tDMRG we calculate the time evolution of the Rényi entanglement entropies. For large subsystems and for any α , their density turns out to be compatible with that of the thermodynamic Rényi entropies.
We study the behaviour of Renyi entropies in a generic thermodynamic macrostate of an integrable model. In the standard quench action approach to quench dynamics, the Renyi entropies may be derived from the overlaps of the initial state with Bethe eigenstates. These overlaps fix the driving term in the thermodynamic Bethe ansatz (TBA) formalism. We show that this driving term can be also reconstructed starting from the macrostate's particle densities. We then compute explicitly the stationary Renyi entropies after the quench from the dimer and the tilted Neel state in XXZ spin chains. For the former state we employ the overlap TBA approach, while for the latter we reconstruct the driving terms from the macrostate. We discuss in full detail the limits that can be analytically handled and we use numerical simulations to check our results against the large time limit of the entanglement entropies.
Abstract We study the behaviour of Rényi entropies in a generic thermodynamic macrostate of an integrable model. In the standard quench action approach to quench dynamics, the Rényi entropies may be derived from the overlaps of the initial state with Bethe eigenstates. These overlaps fix the driving term in the thermodynamic Bethe ansatz (TBA) formalism. We show that this driving term can be also reconstructed starting from the macrostate’s particle densities. We then compute explicitly the stationary Rényi entropies after the quench from the dimer and the tilted Néel state in XXZ spin chains. For the former state we employ the overlap TBA approach, while for the latter we reconstruct the driving terms from the macrostate. We discuss in full detail the limits that can be analytically handled and we use numerical simulations to check our results against the large time limit of the entanglement entropies.
Understanding the entanglement structure of out-of-equilibrium many-body systems is a challenging, yet revealing task. Here, the author investigates the entanglement dynamics after a quench from a piecewise homogeneous state. This is the prototypical setup for studying quantum transport. By using a generalized hydrodynamic approach for integrable models and the quasiparticle picture for the entanglement dynamics, he conjectures a formula for the entanglement production rate after joining two semi-infinite homogeneous states, as well as for the steady-state entanglement entropy of a finite region. Interestingly, both quantities are determined by the physics, describing the interface between the two reservoirs.
We investigate the dynamics of the XXZ spin chain after a geometric quench, which is realized by connecting two half chains prepared in their ground states with zero and maximum magnetizations, respectively. The profiles of magnetization after the subsequent time evolution are studied numerically by density-matrix renormalization group methods, and a comparison to the predictions of generalized hydrodynamics yields a very good agreement. We also calculate the profiles of entanglement entropy and propose an ansatz for the noninteracting XX case, based on arguments from conformal field theory. In the general interacting case, the propagation of the entropy front is studied numerically both before and after the reflection from the chain boundaries. Finally, our results for the magnetization fluctuations indicate a leading order proportionality relation to the entanglement entropy.
The time evolution of the entanglement entropy in non-equilibrium quantum systems provides crucial information about the structure of the time-dependent state. For quantum quench protocols, by combining a quasiparticle picture for the entanglement spreading with the exact knowledge of the stationary state provided by Bethe ansatz, it is possible to obtain an exact and analytic description of the evolution of the entanglement entropy. Here we discuss the application of these ideas to several integrable models. First we show that for non-interacting systems, both bosonic and fermionic, the exact time-dependence of the entanglement entropy can be derived by elementary techniques and without solving the dynamics. We then provide exact results for interacting spin chains that are carefully tested against numerical simulations. Finally, we apply this method to integrable one-dimensional Bose gases (Lieb-Liniger model) both in the attractive and repulsive regimes. We highlight a peculiar behaviour of the entanglement entropy due to the absence of a maximum velocity of excitations.