The classical-quantum limit
- URL: http://arxiv.org/abs/2310.18271v1
- Date: Fri, 27 Oct 2023 16:58:33 GMT
- Title: The classical-quantum limit
- Authors: Isaac Layton, Jonathan Oppenheim
- Abstract summary: The standard notion of a classical limit, represented schematically by $hbarrightarrow 0$, provides a method for approximating a quantum system by a classical one.
Denoting the decoherence time $tau$, we demonstrate that a double scaling limit in which $hbar rightarrow 0$ and $tau rightarrow 0$ remains fixed leads to an irreversible open-system evolution.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: The standard notion of a classical limit, represented schematically by
$\hbar\rightarrow 0$, provides a method for approximating a quantum system by a
classical one. In this work we explain why the standard classical limit fails
when applied to subsystems, and show how one may resolve this by explicitly
modelling the decoherence of a subsystem by its environment. Denoting the
decoherence time $\tau$, we demonstrate that a double scaling limit in which
$\hbar \rightarrow 0$ and $\tau \rightarrow 0$ such that the ratio $E_f =\hbar
/\tau$ remains fixed leads to an irreversible open-system evolution with
well-defined classical and quantum subsystems. The main technical result is
showing that, for arbitrary Hamiltonians, the generators of partial versions of
the Wigner, Husimi and Glauber-Sudarshan quasiprobability distributions may all
be mapped in the above double scaling limit to the same completely-positive
classical-quantum generator. This provides a regime in which one can study
effective and consistent classical-quantum dynamics.
Related papers
- Quantum vs. classical $P$-divisibility [0.0]
$P$-divisibility is a central concept in both classical and quantum non-Markovian processes.
We show that loss of classical $P$-divisibility can originate from the classical reduction of a purely dissipative $P$-divisible quantum dynamics.
arXiv Detail & Related papers (2024-05-09T14:20:54Z) - Chaos and quantization of the three-particle generic
Fermi-Pasta-Ulam-Tsingou model II: phenomenology of quantum eigenstates [5.387047563972287]
We study the phenomenology of quantum eigenstates in the three-particle FPUT model.
We find that in the mixed-type system, the fraction of mixed eigenstates in an energy shell shows a power-law decay with respect to the decreasing Planck constant.
In the general case which is fully chaotic, the maximally localized state is influenced by the stable and unstable manifold of the saddles.
arXiv Detail & Related papers (2024-01-23T19:51:58Z) - Mixed eigenstates in the Dicke model: Statistics and power-law decay of
the relative proportion in the semiclassical limit [8.437514200532176]
We show how mixed eigenstates vary with approaching the semiclassical limit in mixed-type many-body quantum systems.
Using the Husimi function, we show that the eigenstates of the Dicke model with mixed-type classical phase space can be classified into different types.
arXiv Detail & Related papers (2023-09-21T02:31:21Z) - The $\hbar\to 0$ limit of open quantum systems with general Lindbladians: vanishing noise ensures classicality beyond the Ehrenfest time [1.497411457359581]
Quantum and classical systems evolving under the same formal Hamiltonian $H$ may exhibit dramatically different behavior after the Ehrenfest timescale.
Coupling the system to a Markovian environment results in a Lindblad equation for the quantum evolution.
arXiv Detail & Related papers (2023-07-07T17:01:23Z) - Decoherence ensures classicality beyond the Ehrenfest time as $\hbar \to
0$ [1.9499120576896227]
In closed quantum systems, wavepackets can spread exponentially in time due to chaos.
A weakly coupled environment is conjectured to decohere the system and restore the quantum-classical correspondence.
We prove the quantum and classical evolutions are close whenever the strength of the environment-induced diffusion exceeds a threshold.
arXiv Detail & Related papers (2023-06-23T18:01:53Z) - Testing the quantum nature of gravity without entanglement [5.461938536945723]
Given a unitary evolution $U$, how well can $U$ be simulated by local operations and classical communication (LOCC) on that ensemble?
We establish a general, efficiently computable upper bound on the maximal LOCC simulation fidelity.
We then apply our findings to the fundamental setting where $U$ implements a quantum Newtonian Hamiltonian over a gravitationally interacting system.
arXiv Detail & Related papers (2023-02-06T19:22:48Z) - Correspondence between open bosonic systems and stochastic differential
equations [77.34726150561087]
We show that there can also be an exact correspondence at finite $n$ when the bosonic system is generalized to include interactions with the environment.
A particular system with the form of a discrete nonlinear Schr"odinger equation is analyzed in more detail.
arXiv Detail & Related papers (2023-02-03T19:17:37Z) - Defining the semiclassical limit of the quantum Rabi Hamiltonian [0.0]
A formalism for deriving the semiclassical model directly from the quantum Hamiltonian is developed here.
It provides a framework for studying the quantum-to-classical transition, with potential applications in quantum technologies.
arXiv Detail & Related papers (2022-03-31T16:15:57Z) - Fragility to quantum fluctuations of classical Hamiltonian period
doubling [0.0]
We add quantum fluctuations to a classical period-doubling Hamiltonian time crystal, replacing the $N$ classical interacting angular momenta with quantum spins of size $l$.
The full permutation symmetry of the Hamiltonian allows a mapping to a bosonic model and the application of exact diagonalization for quite large system size.
arXiv Detail & Related papers (2021-08-25T18:02:57Z) - Classical non-equilibrium statistical mechanics and an "open system
dynamics" perspective on quantum-classical analogy [4.592848943542229]
We develop a time-local equation of motion using Green's functions and a series expansion method.
We compare this equation of motion with its supposed quantum counterpart, namely the quantum master equation.
We notice an apparent exception to QCA in this case, as the first-order classical equation of motion derived herein contains a term that does not appear to have a quantum analogue.
arXiv Detail & Related papers (2020-05-18T13:49:13Z) - From a quantum theory to a classical one [117.44028458220427]
We present and discuss a formal approach for describing the quantum to classical crossover.
The method was originally introduced by L. Yaffe in 1982 for tackling large-$N$ quantum field theories.
arXiv Detail & Related papers (2020-04-01T09:16:38Z)
This list is automatically generated from the titles and abstracts of the papers in this site.
This site does not guarantee the quality of this site (including all information) and is not responsible for any consequences.