Equilibration of quantum cat states

We study the equilibration properties of isolated ergodic quantum systems initially prepared in a cat state, i.e a macroscopic quantum superposition of states. Our main result consists in showing that, even though decoherence is at work in the mean, there exists a remnant of the initial quantum coherences visible in the strength of the fluctuations of the steady state. We back-up our analysis with numerical results obtained on the XXX spin chain with a random field along the z-axis in the ergodic regime and find good qualitative and quantitative agreement with the theory. We also present and discuss a framework where equilibrium quantities can be computed from general statistical ensembles without relying on microscopic details about the initial state, akin to the eigenstate thermalization hypothesis.We study the equilibration properties of isolated ergodic quantum systems initially prepared in a cat state, i.e a macroscopic quantum superposition of states. Our main result consists in showing that, even though decoherence is at work in the mean, there exists a remnant of the initial quantum coherences visible in the strength of the fluctuations of the steady state. We back-up our analysis with numerical results obtained on the XXX spin chain with a random field along the z-axis in the ergodic regime and find good qualitative and quantitative agreement with the theory. We also present and discuss a framework where equilibrium quantities can be computed from general statistical ensembles without relying on microscopic details about the initial state, akin to the eigenstate thermalization hypothesis.

arXiv:2003.04702SciPost PhysicsJul 8, 20202 citations

Disappearance of macroscopic superpositions in perfectly isolated systems

Chae-Yeun Park, Hyunseok Jeong

Schrödinger's illustration of an imaginary cat in a box, neither alive nor dead, leads to a question of whether and how long a macroscopic quantum superposition can exist in various situations. It is well known that a macroscopic superposition is destroyed very quickly by environmental effects called decoherence. On the contrary, it is often believed that a macroscopic superposition continues to "survive" if it is ideally isolated from its environment. In this paper, using a well-established measure of macroscopic superpositions and the eigenstate thermalization hypothesis, we show that macroscopic superpositions even in ideally closed systems are destroyed by thermalization processes. We further investigate specific examples of a disordered Heisenberg spin chain varied between the thermalization phase and the many-body localized (MBL) phase. This leads to consistent results; initial macroscopic superpositions disappear under thermalization while they may be preserved in the MBL phase in which thermalization does not occur.Schrödinger's illustration of an imaginary cat in a box, neither alive nor dead, leads to a question of whether and how long a macroscopic quantum superposition can exist in various situations. It is well known that a macroscopic superposition is destroyed very quickly by environmental effects called decoherence. On the contrary, it is often believed that a macroscopic superposition continues to "survive" if it is ideally isolated from its environment. In this paper, using a well-established measure of macroscopic superpositions and the eigenstate thermalization hypothesis, we show that macroscopic superpositions even in ideally closed systems are destroyed by thermalization processes. We further investigate specific examples of a disordered Heisenberg spin chain varied between the thermalization phase and the many-body localized (MBL) phase. This leads to consistent results; initial macroscopic superpositions disappear under thermalization while they may be preserved in the MBL phase in which thermalization does not occur.

arXiv:1606.07213Jun 23, 20161 citation

Equilibration properties of small quantum systems: further examples

J. M. Luck

It has been proposed to investigate the equilibration properties of a small isolated quantum system by means of the matrix of asymptotic transition probabilities in some preferential basis. The trace $T$ of this matrix measures the degree of equilibration of the system prepared in a typical state of the preferential basis. This quantity may vary between unity (ideal equilibration) and the dimension $N$ of the Hilbert space (no equilibration at all). Here we analyze several examples of simple systems where the behavior of $T$ can be investigated by analytical means. We first study the statistics of $T$ when the Hamiltonian governing the dynamics is random and drawn from a distribution invariant under the group U $(N)$ or O $(N)$ . We then investigate a quantum spin $S$ in a tilted magnetic field making an arbitrary angle with the preferred quantization axis, as well as a tight-binding particle on a finite electrified chain. The last two cases provide examples of the interesting situation where varying a system parameter -- such as the tilt angle or the electric field -- through some scaling regime induces a continuous transition from good to bad equilibration properties.It has been proposed to investigate the equilibration properties of a small isolated quantum system by means of the matrix of asymptotic transition probabilities in some preferential basis. The trace $T$ of this matrix measures the degree of equilibration of the system prepared in a typical state of the preferential basis. This quantity may vary between unity (ideal equilibration) and the dimension $N$ of the Hilbert space (no equilibration at all). Here we analyze several examples of simple systems where the behavior of $T$ can be investigated by analytical means. We first study the statistics of $T$ when the Hamiltonian governing the dynamics is random and drawn from a distribution invariant under the group U$(N)$ or O$(N)$. We then investigate a quantum spin $S$ in a tilted magnetic field making an arbitrary angle with the preferred quantization axis, as well as a tight-binding particle on a finite electrified chain. The last two cases provide examples of the interesting situation where varying a system parameter -- such as the tilt angle or the electric field -- through some scaling regime induces a continuous transition from good to bad equilibration properties.

Mar 7, 20172 citations

Equilibration and the eigenstate thermalization hypothesis as limits to observing macroscopic quantum superpositions

Gabriel Dias Carvalho, Pedro S. Correia, Thiago R. de Oliveira

Macroscopic quantum superpositions are widely believed to be unobservable because large systems cannot be perfectly isolated from their environments. Here, we show that even under perfect isolation, intrinsic unitary dynamics in generic many-body systems, as analyzed through the eigenstate thermalization hypothesis and random matrix theory, can suppress the observable signatures of macroscopic coherence. Using the Greenberger-Horne-Zeilinger (GHZ) state as a representative example, we demonstrate that while fully correlated measurements can initially distinguish a macroscopic superposition from its corresponding classical mixture, generic many-body evolution renders them operationally indistinguishable for most times. By analyzing both distinguishability measures and established quantifiers of macroscopic quantumness, we find that equilibration not only hides coherence from accessible observables but also suppresses the corresponding signatures of macroscopic quantumness, in particular within the additive-local framework considered here. These results identify unitary thermalization, independent of environmental decoherence, as a fundamental mechanism that limits the observation of macroscopic quantum effects.Macroscopic quantum superpositions are widely believed to be unobservable because large systems cannot be perfectly isolated from their environments. Here, we show that even under perfect isolation, intrinsic unitary dynamics in generic many-body systems, as analyzed through the eigenstate thermalization hypothesis and random matrix theory, can suppress the observable signatures of macroscopic coherence. Using the Greenberger-Horne-Zeilinger (GHZ) state as a representative example, we demonstrate that while fully correlated measurements can initially distinguish a macroscopic superposition from its corresponding classical mixture, generic many-body evolution renders them operationally indistinguishable for most times. By analyzing both distinguishability measures and established quantifiers of macroscopic quantumness, we find that equilibration not only hides coherence from accessible observables but also suppresses the corresponding signatures of macroscopic quantumness, in particular within the additive-local framework considered here. These results identify unitary thermalization, independent of environmental decoherence, as a fundamental mechanism that limits the observation of macroscopic quantum effects.

quant-pharXiv:2512.11522Physical Review ADec 15, 20250 citations

Disappearance of macroscopic superpositions in perfectly isolated systems by thermalization processes

Chae-Yeun Park, Hyunseok Jeong

Schr\odinger's illustration of an imaginary cat in a box, neither alive nor dead, leads to a question of whether and how long a macroscopic quantum superposition can exist in various situations. It is well known that a macroscopic superposition is destroyed very quickly by environmental effects called decoherence. On the contrary, it is often believed that a macroscopic superposition continues to survive if it is ideally isolated from its environment. In this paper, using a well-established measure of macroscopic superpositions and the eigenstate thermalization hypothesis, we show that macroscopic superpositions even in ideally closed systems are destroyed by thermalization processes. We further investigate specific examples of a disordered Heisenberg spin chain varied between the thermalization phase and the many-body localization (MBL) phase. Consistent results are obtained that initial macroscopic superpositions that undergo thermalization disappear while they are preserved in the MBL phase in which thermalization does not occur.Schr\odinger's illustration of an imaginary cat in a box, neither alive nor dead, leads to a question of whether and how long a macroscopic quantum superposition can exist in various situations. It is well known that a macroscopic superposition is destroyed very quickly by environmental effects called decoherence. On the contrary, it is often believed that a macroscopic superposition continues to survive if it is ideally isolated from its environment. In this paper, using a well-established measure of macroscopic superpositions and the eigenstate thermalization hypothesis, we show that macroscopic superpositions even in ideally closed systems are destroyed by thermalization processes. We further investigate specific examples of a disordered Heisenberg spin chain varied between the thermalization phase and the many-body localization (MBL) phase. Consistent results are obtained that initial macroscopic superpositions that undergo thermalization disappear while they are preserved in the MBL phase in which thermalization does not occur.

Jun 23, 20161 citation

Equilibration properties of small quantum systems: further examples

J. M. Luck

Abstract It has been proposed to investigate the equilibration properties of a small isolated quantum system by means of the matrix of asymptotic transition probabilities in some preferential basis. The trace T of this matrix measures the degree of equilibration of the system prepared in a typical state of the preferential basis. This quantity may vary between unity (ideal equilibration) and the dimension N of the Hilbert space (no equilibration at all). Here we analyze several examples of simple systems where the behavior of T can be investigated by analytical means. We first study the statistics of T when the Hamiltonian governing the dynamics is random and drawn from a distribution invariant under the group U ( N ) or O ( N ) . We then investigate a quantum spin S in a tilted magnetic field making an arbitrary angle with the preferred quantization axis, as well as a tight-binding particle on a finite electrified chain. The last two cases provide examples of the interesting situation where varying a system parameter—such as the tilt angle or the electric field—through some scaling regime induces a continuous crossover from good to bad equilibration properties.Abstract It has been proposed to investigate the equilibration properties of a small isolated quantum system by means of the matrix of asymptotic transition probabilities in some preferential basis. The trace T of this matrix measures the degree of equilibration of the system prepared in a typical state of the preferential basis. This quantity may vary between unity (ideal equilibration) and the dimension N of the Hilbert space (no equilibration at all). Here we analyze several examples of simple systems where the behavior of T can be investigated by analytical means. We first study the statistics of T when the Hamiltonian governing the dynamics is random and drawn from a distribution invariant under the group U ( N ) or O ( N ) . We then investigate a quantum spin S in a tilted magnetic field making an arbitrary angle with the preferred quantization axis, as well as a tight-binding particle on a finite electrified chain. The last two cases provide examples of the interesting situation where varying a system parameter—such as the tilt angle or the electric field—through some scaling regime induces a continuous crossover from good to bad equilibration properties.

arXiv:1702.05909Journal of Physics A Mathematical and TheoreticalJul 13, 20172 citations

It has been proposed to investigate the equilibration properties of a small isolated quantum system by means of the matrix of asymptotic transition probabilities in some preferential basis. The trace

T

of this matrix measures the degree of equilibration of the system prepared in a typical state of the preferential basis. This quantity may vary between unity (ideal equilibration) and the dimension

N

of the Hilbert space (no equilibration at all). Here we analyze several examples of simple systems where the behavior of

T

can be investigated by analytical means. We first study the statistics of

T

when the Hamiltonian governing the dynamics is random and drawn from a distribution invariant under the group U

(N)

or O

(N)

. We then investigate a quantum spin

S

in a tilted magnetic field making an arbitrary angle with the preferred quantization axis, as well as a tight-binding particle on a finite electrified chain. The last two cases provide examples of the interesting situation where varying a system parameter -- such as the tilt angle or the electric field -- through some scaling regime induces a continuous transition from good to bad equilibration properties.