Horizon thermalization of Kerr black hole through local instability
- URL: http://arxiv.org/abs/2103.11613v2
- Date: Mon, 10 Jan 2022 11:42:30 GMT
- Title: Horizon thermalization of Kerr black hole through local instability
- Authors: Surojit Dalui, Bibhas Ranjan Majhi
- Abstract summary: We show that for a chargeless massless particle, the near horizon radial motion in Kerr spacetime, like SSS BH, can be locally unstable.
It again confirms that near horizon instability is liable for its own temperature and moreover generalizes the validity of our conjectured mechanism for the black hole horizon thermalization.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: The validity of our already proposed conjecture -- {\it horizon creates a
local instability which acts as the source of the quantum temperature of black
hole} -- is being tested here for Kerr black hole. Earlier this has been
explicitly shown for spherically symmetric static black hole (SSS BH). The more
realistic situation like Kerr spacetime, being stationary and axisymmetric, is
a non-trivial example to analyze. We show that for a chargeless massless
particle, the near horizon radial motion in Kerr spacetime, like SSS BH, can be
locally unstable. The radial contribution in the corresponding Hamiltonian is
$\sim xp$ kind, where $p$ is the canonical momentum and $x$ is its conjugate
position of particle. Finally we show that the horizon thermalization can be
explained through this Hamiltonian when one dose a semi-classical analysis. It
again confirms that near horizon instability is liable for its own temperature
and moreover generalizes the validity of our conjectured mechanism for the
black hole horizon thermalization.
Related papers
- Singular Excitement Beyond the Horizon of a Rotating Black Hole [4.003194245289446]
We numerically compute the detector's transition rate for different values of black hole mass, black hole angular momentum, detector energy gap, and field boundary conditions at infinity.
Our results lead to a more generalized description of the behaviour of particle detectors in BTZ black hole spacetime.
arXiv Detail & Related papers (2024-07-01T18:00:01Z) - Decoherence by warm horizons [12.14598582153305]
We map the DSW set-up onto a worldline-localized model resembling an Unruh-DeWitt particle detector.
We show that the Unruh effect is the only quantum mechanical effect underlying these random forces.
arXiv Detail & Related papers (2024-05-01T18:39:00Z) - 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) - Photon topology [22.20907440445493]
We show that there are no photons with $boldsymbolk=0$, creating a hole in momentum space.
While the set of all photons forms a trivial vector bundle $gamma$ over this momentum space, the $R$- and $L$-photons form topologically nontrivial subbundles.
We also demonstrate that the spin-Chern number of photons is not a purely topological quantity.
arXiv Detail & Related papers (2023-08-22T03:05:37Z) - Thermality of horizon through near horizon instability: a path integral
approach [0.0]
The near horizon Hamiltonian of a chargeless outgoing particle, for its particular motion in static as well as stationary black holes, is effectively $sim XP$ kind.
We calculate the effective path corresponding to its Schrodinger version of Hamiltonian through the path integral approach.
In both ways, we identify the correct expression of Hawking temperature.
arXiv Detail & Related papers (2022-10-08T15:52:49Z) - A New Look at the $C^{0}$-formulation of the Strong Cosmic Censorship
Conjecture [68.8204255655161]
We argue that for generic black hole parameters as initial conditions for Einstein equations, the metric is $C0$-extendable to a larger Lorentzian manifold.
We prove it violates the "complexity=volume" conjecture for a low-temperature hyperbolic AdS$_d+1$ black hole dual to a CFT living on a ($d-1$)-dimensional hyperboloid $H_d-1$.
arXiv Detail & Related papers (2022-06-17T12:14:33Z) - Near horizon aspects (and beyond) of acceleration radiation of an atom
falling into a large class of static spherically symmetric black hole
geometries [0.29998889086656577]
We consider the near horizon aspects (and beyond) of a black hole metric, which belongs to a large class of static spherically symmetric black holes.
For the next part of our analysis, we have observed the horizon brightened acceleration radiation entropy (HBAR) for a Garfinkle-Horowitz-Strominger (GHS) black hole.
arXiv Detail & Related papers (2022-05-20T11:41:04Z) - Gravitational orbits, double-twist mirage, and many-body scars [77.34726150561087]
We explore the implications of stable gravitational orbits around an AdS black hole for the boundary conformal field theory.
The orbits are long-lived states that eventually decay due to gravitational radiation and tunneling.
arXiv Detail & Related papers (2022-04-20T19:18:05Z) - Quantum simulation of Hawking radiation and curved spacetime with a
superconducting on-chip black hole [18.605453401936643]
We report a fermionic lattice-model-type realization of an analogue black hole by using a chain of 10 superconducting transmon qubits with interactions mediated by 9 transmon-type tunable couplers.
The quantum walks of quasi-particle in the curved spacetime reflect the gravitational effect near the black hole, resulting in the behaviour of stimulated Hawking radiation.
arXiv Detail & Related papers (2021-11-22T10:17:23Z) - BMS Goldstone modes near the horizon of a Kerr black hole are thermal [0.0]
Near horizon Bondi-Metzner-Sachs (BMS) like symmetry is spontaneously broken by the black hole background itself and hence gives rise to Goldstone mode.
The associated Goldstone mode for the near horizon BMS like symmetry of a Schwarzschild black hole was found to behave like inverted harmonic oscillators.
arXiv Detail & Related papers (2021-07-26T12:31:24Z) - Is instability near a black hole key for "thermalization'' of its
horizon? [0.0]
Near horizon Hamiltonian for a massless, chargeless particle is $xp$ type.
This is unstable in nature and so the horizon can induce instability in a system.
The particle in turn finds the horizon thermal when it interacts with it.
arXiv Detail & Related papers (2021-01-12T13:05:37Z)
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.