Quantum power: a Lorentz invariant approach to Hawking radiation
- URL: http://arxiv.org/abs/2111.15148v1
- Date: Tue, 30 Nov 2021 06:13:34 GMT
- Title: Quantum power: a Lorentz invariant approach to Hawking radiation
- Authors: Michael R.R. Good and Eric V. Linder
- Abstract summary: An accelerating mirror with a prolonged metastable acceleration plateau can provide a unitary, thermal, energy-conserved analog model for black hole decay.
We show that an accelerating mirror with a prolonged metastable acceleration plateau can provide a unitary, thermal, energy-conserved analog model for black hole decay.
- Score: 0.0
- License: http://creativecommons.org/licenses/by/4.0/
- Abstract: Particle radiation from black holes has an observed emission power depending
on the surface gravity $\kappa = c^4/(4GM)$ as \begin{equation}\nonumber
P_{\textrm{black hole}} \sim \frac{\hbar \kappa^2}{6\pi c^2} = \frac{\hbar
c^6}{96\pi G^2 M^2}\,,\end{equation} while both the radiation from accelerating
particles and moving mirrors (accelerating boundaries) obey similar
relativistic Larmor powers, \begin{equation}\nonumber P_{\textrm{electron}}=
\frac{q^2\alpha^2}{6\pi \epsilon_0 c^3}\,, \quad P_{\textrm{mirror}}
=\frac{\hbar \alpha^2}{6\pi c^2}\,, \end{equation} where $\alpha$ is the
Lorentz invariant proper acceleration. This equivalence between the Lorentz
invariant powers suggests a close relation that could be used to understand
black hole radiation. We show that an accelerating mirror with a prolonged
metastable acceleration plateau can provide a unitary, thermal,
energy-conserved analog model for black hole decay.
Related papers
- Klein-Gordon oscillators and Bergman spaces [55.2480439325792]
We consider classical and quantum dynamics of relativistic oscillator in Minkowski space $mathbbR3,1$.
The general solution of this model is given by functions from the weighted Bergman space of square-integrable holomorphic (for particles) and antiholomorphic functions on the K"ahler-Einstein manifold $Z_6$.
arXiv Detail & Related papers (2024-05-23T09:20:56Z) - Vacuum Force and Confinement [65.268245109828]
We show that confinement of quarks and gluons can be explained by their interaction with the vacuum Abelian gauge field $A_sfvac$.
arXiv Detail & Related papers (2024-02-09T13:42:34Z) - Ultracold Neutrons in the Low Curvature Limit: Remarks on the
post-Newtonian effects [49.1574468325115]
We apply a perturbative scheme to derive the non-relativistic Schr"odinger equation in curved spacetime.
We calculate the next-to-leading order corrections to the neutron's energy spectrum.
While the current precision for observations of ultracold neutrons may not yet enable to probe them, they could still be relevant in the future or in alternative circumstances.
arXiv Detail & Related papers (2023-12-30T16:45:56Z) - On the relativistic quantum mechanics of a photon between two electrons
in 1+1 dimensions [0.0]
A Lorentz-covariant system of wave equations is formulated for a quantum-mechanical three-body system in one space dimension, comprised of one photon and two identical massive spin one-half Dirac particles.
Manifest covariance is achieved using Dirac's formalism of multi-time wave functions.
arXiv Detail & Related papers (2023-12-10T22:21:33Z) - Small-time controllability for the nonlinear Schr\"odinger equation on
$\mathbb{R}^N$ via bilinear electromagnetic fields [55.2480439325792]
We address the small-time controllability problem for a nonlinear Schr"odinger equation (NLS) on $mathbbRN$ in the presence of magnetic and electric external fields.
In detail, we study when it is possible to control the dynamics of (NLS) as fast as desired via sufficiently large control signals.
arXiv Detail & Related papers (2023-07-28T21:30:44Z) - Signatures of quantum geometry from exponential corrections to the black hole entropy [0.10713888959520207]
We obtain the possible form of the spacetime geometry from the entropy of the black hole for a given horizon radius.
Remarkably, the black hole geometry reconstructed has striking similarities to that of noncommutative-inspired Schwarzschild black holes.
arXiv Detail & Related papers (2022-09-27T13:40:55Z) - Coherent transfer of the transverse momentum of an optical vortex beam
to the motion of a single trapped ion [22.42090005507693]
We demonstrate the excitation, using a structured light beam carrying orbital angular momentum, of the center of mass motion of a single atom.
We characterize the coherent interaction by an effective transverse Lamb-Dicke factor $etamathrmexp_perp62(5)$ which is in agreement with our theoretical prediction $etamathrmtheo_perp57(1)$
arXiv Detail & Related papers (2022-06-10T06:15:08Z) - On quantum algorithms for the Schr\"odinger equation in the
semi-classical regime [27.175719898694073]
We consider Schr"odinger's equation in the semi-classical regime.
Such a Schr"odinger equation finds many applications, including in Born-Oppenheimer molecular dynamics and Ehrenfest dynamics.
arXiv Detail & Related papers (2021-12-25T20:01:54Z) - Schr\"odinger equation in a general curved space-time geometry [0.0]
We consider relativistic quantum field theory in the presence of an external electric potential in a general curved space-time geometry.
We calculate the leading correction due to the curvature of the space-time geometry to the Schr"odinger equation.
We then compute the non-vanishing probability of excitation for a hydrogen atom that falls in or is scattered by a general Schwarzschild black hole.
arXiv Detail & Related papers (2021-05-26T18:47:44Z) - Accelerating boundary analog of a Kerr black hole [0.0]
The betaoliubov coefficients reveal the particle spectrum is a Planck distribution at late times with temperature cooler than a Schwarzschild black hole.
The quantum stress tensor indicates a constant emission of energy flux at late times consistent with eternal thermal equilibrium.
arXiv Detail & Related papers (2020-06-02T02:25:42Z) - The $E$, the $A$, the Dirac equation and the propagator [0.0]
Dirac equation in the presence of electromagnetic field is equation of Dirac spinor, $psi$, satisfying $ihbar fracpartial psipartial t.
We say that Dirac equation in the presence of electromagnetic field is equation of Dirac spinor, $psi$, satisfying $ihbar fracpartial psipartial t.
arXiv Detail & Related papers (2018-01-25T13:24:32Z)
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.