Gaussian work extraction from random Gaussian states is nearly
impossible
- URL: http://arxiv.org/abs/2212.03492v2
- Date: Tue, 18 Jul 2023 10:21:23 GMT
- Title: Gaussian work extraction from random Gaussian states is nearly
impossible
- Authors: Uttam Singh, Jaros{\l}aw K. Korbicz, Nicolas J. Cerf
- Abstract summary: A key resource in thermodynamics is the extractable work, forming the backbone of thermal engines.
We show that Gaussian states are typically useless for Gaussian work extraction.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: Quantum thermodynamics can be naturally phrased as a theory of quantum state
transformation and energy exchange for small-scale quantum systems undergoing
thermodynamical processes, thereby making the resource theoretical approach
very well suited. A key resource in thermodynamics is the extractable work,
forming the backbone of thermal engines. Therefore it is of interest to
characterize quantum states based on their ability to serve as a source of
work. From a near-term perspective, quantum optical setups turn out to be ideal
test beds for quantum thermodynamics; so it is important to assess work
extraction from quantum optical states. Here, we show that Gaussian states are
typically useless for Gaussian work extraction. More specifically, by
exploiting the ``concentration of measure'' phenomenon, we prove that the
probability that the Gaussian extractable work from a zero-mean energy-bounded
multimode random Gaussian state is nonzero is exponentially small. This result
can be thought of as an $\epsilon$-no-go theorem for work extraction from
Gaussian states under Gaussian unitaries, thereby revealing a fundamental
limitation on the quantum thermodynamical usefulness of Gaussian components.
Related papers
- Quantumness Speeds up Quantum Thermodynamics Processes [1.3597551064547502]
We show the coherence of quantum systems can speed up work extracting with respect to some cyclic evolution beyond all incoherent states.
We further show the genuine entanglement of quantum systems may speed up work extracting beyond any bi-separablestates.
arXiv Detail & Related papers (2024-06-19T08:52:19Z) - Quantum non-Markovianity, quantum coherence and extractable work in a
general quantum process [0.0]
Key concept in quantum thermodynamics is extractable work, which specifies the maximum amount of work that can be extracted from a quantum system.
Different quantities are used to measure extractable work, the most prevalent of which are ergotropy and the difference between the non-equilibrium and equilibrium quantum free energy.
We investigate the evolution of extractable work when an open quantum system goes through a general quantum process described by a completely-positive and trace-preserving dynamical map.
arXiv Detail & Related papers (2023-09-10T11:05:35Z) - Sparse random Hamiltonians are quantumly easy [105.6788971265845]
A candidate application for quantum computers is to simulate the low-temperature properties of quantum systems.
This paper shows that, for most random Hamiltonians, the maximally mixed state is a sufficiently good trial state.
Phase estimation efficiently prepares states with energy arbitrarily close to the ground energy.
arXiv Detail & Related papers (2023-02-07T10:57:36Z) - Work extraction from unknown quantum sources [0.0]
In quantum physics, ergotropy measures the amount of work extractable under cyclic Hamiltonian control.
Here, we derive a new notion of ergotropy applicable when nothing is known about the quantum states produced by the source.
We find that in this case the extracted work is defined by the Boltzmann and observational entropy, in cases where the measurement outcomes are, or are not, used in the work extraction.
arXiv Detail & Related papers (2022-09-22T15:07:04Z) - Demonstrating Quantum Microscopic Reversibility Using Coherent States of
Light [58.8645797643406]
We propose and experimentally test a quantum generalization of the microscopic reversibility when a quantum system interacts with a heat bath.
We verify that the quantum modification for the principle of microscopic reversibility is critical in the low-temperature limit.
arXiv Detail & Related papers (2022-05-26T00:25:29Z) - Correspondence Between the Energy Equipartition Theorem in Classical
Mechanics and its Phase-Space Formulation in Quantum Mechanics [62.997667081978825]
In quantum mechanics, the energy per degree of freedom is not equally distributed.
We show that in the high-temperature regime, the classical result is recovered.
arXiv Detail & Related papers (2022-05-24T20:51:03Z) - Maximum entropy quantum state distributions [58.720142291102135]
We go beyond traditional thermodynamics and condition on the full distribution of the conserved quantities.
The result are quantum state distributions whose deviations from thermal states' get more pronounced in the limit of wide input distributions.
arXiv Detail & Related papers (2022-03-23T17:42:34Z) - Dissipative evolution of quantum Gaussian states [68.8204255655161]
We derive a new model of dissipative time evolution based on unitary Lindblad operators.
As we demonstrate, the considered evolution proves useful both as a description for random scattering and as a tool in dissipator engineering.
arXiv Detail & Related papers (2021-05-26T16:03:34Z) - Taking the temperature of a pure quantum state [55.41644538483948]
Temperature is a deceptively simple concept that still raises deep questions at the forefront of quantum physics research.
We propose a scheme to measure the temperature of such pure states through quantum interference.
arXiv Detail & Related papers (2021-03-30T18:18:37Z) - Strong Coupling Quantum Thermodynamics with Renormalized Hamiltonian and
Temperature [2.542198147027801]
We develop strong coupling quantum thermodynamics based on the solution of the exact master equation.
We find that both the Hamiltonian and the temperature must be renormalized due to the system-reservoir couplings.
With the renormalized Hamiltonian and temperature, the exact steady state of open quantum systems can be expressed as a standard Gibbs state.
arXiv Detail & Related papers (2020-10-05T07:34:26Z) - The First Law of Quantum Field Thermodynamics [0.0]
We show that the most common definitions used in finite-dimensional quantum systems cannot be applied to quantum field theory (QFT)
We propose work distributions that are compatible with QFT and we show that they satisfy the first law of thermodynamics up to second moments.
arXiv Detail & Related papers (2020-08-20T18:16:26Z)
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.