Entanglement asymmetry and quantum Mpemba effect in the XY spin chain
Sara Murciano,
Filiberto Ares,
Israel Klich
et al.
Abstract:Entanglement asymmetry is a quantity recently introduced to measure how much a symmetry is broken in a part of an extended quantum system. It has been employed to analyze the non-equilibrium dynamics of a broken symmetry after a global quantum quench with a Hamiltonian that preserves it. In this work, we carry out a comprehensive analysis of the entanglement asymmetry at equilibrium taking the ground state of the XY spin chain, which breaks the U(1) particle number symmetry, and provide a physical interpretati… Show more
“…Classical Mpemba effect was observed also in several other systems, such as clathrate hydrates [16], magnetic alloys [17], carbon nanotube resonators [18], granular gases [19], colloidal systems [20] or dilute atomic gases [21]. A microscopic explanation of the quantum Mpemba effect in both interacting and free integrable spin chains has been provided in [5] (see also [9] for a further study of the asymmetry in free integrable quantum systems).…”
Section: Introductionmentioning
confidence: 83%
“…from the tilted ferromagnetic state [1], and, more in general, from the ground state of the XY spin chain [9], which does not preserve the transverse magnetization. In these situations, the dynamics determined by a free U (1)-invariant Hamiltonian leads to the symmetry restoration of the U (1) charge in the subsystem.…”
Section: Introductionmentioning
confidence: 98%
“…Indeed, the concepts of symmetry and symmetry-breaking are ubiquitous in Physics. In recent years there has been renewed interest in studying symmetry-breaking both in and out-of-equilibrium systems [1][2][3][4][5][6][7][8][9][10][11]. Let us consider the prototypical setup of the quantum quench [12] in which a system, here a one-dimensional one, is prepared in an initial state and let to evolve under a many-body Hamiltonian H. Let us also assume that the Hamiltonian commutes with a charge operator Q, which generates an Abelian symmetry U (1).…”
Section: Introductionmentioning
confidence: 99%
“…Crucially, the dynamics of the entanglement asymmetry, and the onset of the quantum Mpemba effect, can be understood in the space-time scaling limit (hydrodynamic limit) ℓ, t → ∞ with the ratio t/ℓ fixed. Indeed, the main formula obtained in [1,9] is reminiscent of the socalled quasiparticle picture [26][27][28][29] for the entanglement entropy. Still, a full-fledged quasiparticle picture was not available so far.…”
Section: Introductionmentioning
confidence: 99%
“…Here we first review the results of [1,2,9]. We focus on a dynamics governed by the XX chain, considering quantum quenches from the ground state of the XY chain and the tilted Néel state.…”
Recently, the entanglement asymmetry emerged as an informative tool to understand dynamical symmetry restoration in out-of-equilibrium quantum many-body systems after a quantum quench. For integrable systems the asymmetry can be understood in the space-time scaling limit via the quasiparticle picture, as it was pointed out in Ares et al (2023 Nat. Commun.
14 2036) . However, a quasiparticle picture for quantum quenches from generic initial states was still lacking. Here we conjecture a full-fledged quasiparticle picture for the charged moments of the reduced density matrix, which are the main ingredients to construct the asymmetry. Our formula works for quenches producing entangled multiplets of an arbitrary number of excitations. We benchmark our results in the XX spin chain. First, by using an elementary approach based on the multidimensional stationary phase approximation we provide an ab initio rigorous derivation of the dynamics of the charged moments for the quench treated in Ares et al (2023 SciPost Phys.
15 089). Then, we show that the same results can be straightforwardly obtained within our quasiparticle picture. As a byproduct of our analysis, we obtain a general criterion ensuring a vanishing entanglement asymmetry at long times. Next, by using the Lindblad master equation, we study the effect of gain and loss dissipation on the entanglement asymmetry. Specifically, we investigate the fate of the so-called quantum Mpemba effect (QME) in the presence of dissipation. We show that dissipation can induce QME even if unitary dynamics does not show it, and we provide a quasiparticle-based interpretation of the condition for the QME.
“…Classical Mpemba effect was observed also in several other systems, such as clathrate hydrates [16], magnetic alloys [17], carbon nanotube resonators [18], granular gases [19], colloidal systems [20] or dilute atomic gases [21]. A microscopic explanation of the quantum Mpemba effect in both interacting and free integrable spin chains has been provided in [5] (see also [9] for a further study of the asymmetry in free integrable quantum systems).…”
Section: Introductionmentioning
confidence: 83%
“…from the tilted ferromagnetic state [1], and, more in general, from the ground state of the XY spin chain [9], which does not preserve the transverse magnetization. In these situations, the dynamics determined by a free U (1)-invariant Hamiltonian leads to the symmetry restoration of the U (1) charge in the subsystem.…”
Section: Introductionmentioning
confidence: 98%
“…Indeed, the concepts of symmetry and symmetry-breaking are ubiquitous in Physics. In recent years there has been renewed interest in studying symmetry-breaking both in and out-of-equilibrium systems [1][2][3][4][5][6][7][8][9][10][11]. Let us consider the prototypical setup of the quantum quench [12] in which a system, here a one-dimensional one, is prepared in an initial state and let to evolve under a many-body Hamiltonian H. Let us also assume that the Hamiltonian commutes with a charge operator Q, which generates an Abelian symmetry U (1).…”
Section: Introductionmentioning
confidence: 99%
“…Crucially, the dynamics of the entanglement asymmetry, and the onset of the quantum Mpemba effect, can be understood in the space-time scaling limit (hydrodynamic limit) ℓ, t → ∞ with the ratio t/ℓ fixed. Indeed, the main formula obtained in [1,9] is reminiscent of the socalled quasiparticle picture [26][27][28][29] for the entanglement entropy. Still, a full-fledged quasiparticle picture was not available so far.…”
Section: Introductionmentioning
confidence: 99%
“…Here we first review the results of [1,2,9]. We focus on a dynamics governed by the XX chain, considering quantum quenches from the ground state of the XY chain and the tilted Néel state.…”
Recently, the entanglement asymmetry emerged as an informative tool to understand dynamical symmetry restoration in out-of-equilibrium quantum many-body systems after a quantum quench. For integrable systems the asymmetry can be understood in the space-time scaling limit via the quasiparticle picture, as it was pointed out in Ares et al (2023 Nat. Commun.
14 2036) . However, a quasiparticle picture for quantum quenches from generic initial states was still lacking. Here we conjecture a full-fledged quasiparticle picture for the charged moments of the reduced density matrix, which are the main ingredients to construct the asymmetry. Our formula works for quenches producing entangled multiplets of an arbitrary number of excitations. We benchmark our results in the XX spin chain. First, by using an elementary approach based on the multidimensional stationary phase approximation we provide an ab initio rigorous derivation of the dynamics of the charged moments for the quench treated in Ares et al (2023 SciPost Phys.
15 089). Then, we show that the same results can be straightforwardly obtained within our quasiparticle picture. As a byproduct of our analysis, we obtain a general criterion ensuring a vanishing entanglement asymmetry at long times. Next, by using the Lindblad master equation, we study the effect of gain and loss dissipation on the entanglement asymmetry. Specifically, we investigate the fate of the so-called quantum Mpemba effect (QME) in the presence of dissipation. We show that dissipation can induce QME even if unitary dynamics does not show it, and we provide a quasiparticle-based interpretation of the condition for the QME.
The entanglement asymmetry is an information based observable that quantifies the degree of symmetry breaking in a region of an extended quantum system. We investigate this measure in the ground state of one dimensional critical systems described by a CFT. Employing the correspondence between global symmetries and defects, the analysis of the entanglement asymmetry can be formulated in terms of partition functions on Riemann surfaces with multiple non-topological defect lines inserted at their branch cuts. For large subsystems, these partition functions are determined by the scaling dimension of the defects. This leads to our first main observation: at criticality, the entanglement asymmetry acquires a subleading contribution scaling as log ℓ/ℓ for large subsystem length ℓ. Then, as an illustrative example, we consider the XY spin chain, which has a critical line described by the massless Majorana fermion theory and explicitly breaks the U(1) symmetry associated with rotations about the z-axis. In this situation the corresponding defect is marginal. Leveraging conformal invariance, we relate the scaling dimension of these defects to the ground state energy of the massless Majorana fermion on a circle with equally-spaced point defects. We exploit this mapping to derive our second main result: the exact expression for the scaling dimension associated with n defects of arbitrary strengths. Our result generalizes a known formula for the n = 1 case derived in several previous works. We then use this exact scaling dimension to derive our third main result: the exact prefactor of the log ℓ/ℓ term in the asymmetry of the critical XY chain.
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