On the Phenomenology of Quantum Gravity: Stability Properties of Hawking Radiation in the Presence of Ultraviolet Violation of L
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Phase Transition of Quantum-Corrected Schwarzschild Black Hole in Rainbow Gravity
Physics Letters B 784 (2018) 6–11 Contents lists available at ScienceDirect Physics Letters B www.elsevier.com/locate/physletb Phase transition of quantum-corrected Schwarzschild black hole in rainbow gravity Md. Shahjalal Department of Mathematics, Shahjalal University of Science and Technology, Sylhet-3114, Bangladesh a r t i c l e i n f o a b s t r a c t Article history: The thermodynamic phase transition of Schwarzschild black hole, after employing a quantum correction Received 30 May 2018 to the space–time metric, in the gravity’s rainbow is explored. The rainbow gravity-inspired Hawking Received in revised form 15 July 2018 temperature of the quantum-corrected rainbow Schwarzschild black hole is calculated initially, and then Accepted 16 July 2018 the entropy, the local temperature, and the local energy of the black hole in an isothermal cavity Available online 20 July 2018 are derived. The off-shell free energy is calculated to further investigate the critical behavior, the Editor: B. Grinstein thermodynamic stability, and the phase transition of the black hole. It is evident that the rainbow gravity Keywords: determines the late fate of the black hole as leading to a remnant, the findings of this letter also show Rainbow gravity that a quantum correction to the metric reduces the remnant mass of the Schwarzschild black hole in Black hole thermodynamics comparison with the usual rainbow Schwarzschild black hole. Phase transition © 2018 The Author(s). Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). -
Black Hole Termodinamics and Hawking Radiation
Black hole thermodynamics and Hawking radiation (Just an overview by a non-expert on the field!) Renato Fonseca - 26 March 2018 – for the Journal Club Thermodynamics meets GR • Research in the 70’s convincingly brought together two very different areas of physics: thermodynamics and General Relativity • People realized that black holes (BHs) followed some laws similar to the ones observed in thermodynamics • It was then possible to associate a temperature to BHs. But was this just a coincidence? • No. Hawkings (1975) showed using QFT in curved space that BHs from gravitational collapse radiate as a black body with a certain temperature T Black Holes Schwarzschild metric (for BHs with no spin nor electric charge) • All coordinates (t,r,theta,phi) are what you think they are far from the central mass M • Something funny seems to happen for r=2M. But … locally there is nothing special there (only at r=0): r=0: real/intrinsic singularity r=2M: apparent singularity (can be removed with other coordinates) Important caveat: the Schwarzschild solution is NOT what is called maximal. With coordinates change we can get the Kruskal solution, which is. “Maximal”= ability to continue geodesics until infinity or an intrinsic singularity Schwarzschild metric (for BHs with no spin nor electric charge) • r=2M (event horizon) is not special for its LOCAL properties (curvature, etc) but rather for its GLOBAL properties: r<=2M are closed trapped surfaces which cannot communicate with the outside world [dr/dt=0 at r=2M even for light] Fun fact: for null geodesics (=light) we see that +/- = light going out/in One can even integrate this: t=infinite for even light to fall into the BH! This is what an observatory at infinity sees … (Penrose, 1969) Schwarzschild metric (digression) • But the object itself does fall into the BH. -
Hawking Radiation As Perceived by Different Observers L C Barbado, C Barceló, L J Garay
Hawking radiation as perceived by different observers L C Barbado, C Barceló, L J Garay To cite this version: L C Barbado, C Barceló, L J Garay. Hawking radiation as perceived by different observers. Classical and Quantum Gravity, IOP Publishing, 2011, 10 (12), pp.125021. 10.1088/0264-9381/28/12/125021. hal-00710459 HAL Id: hal-00710459 https://hal.archives-ouvertes.fr/hal-00710459 Submitted on 21 Jun 2012 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Confidential: not for distribution. Submitted to IOP Publishing for peer review 24 March 2011 Hawking radiation as perceived by different observers LCBarbado1,CBarcel´o1 and L J Garay2,3 1 Instituto de Astrof´ısica de Andaluc´ıa(CSIC),GlorietadelaAstronom´ıa, 18008 Granada, Spain 2 Departamento de F´ısica Te´orica II, Universidad Complutense de Madrid, 28040 Madrid, Spain 3 Instituto de Estructura de la Materia (CSIC), Serrano 121, 28006 Madrid, Spain E-mail: [email protected], [email protected], [email protected] Abstract. We use a method recently introduced in Barcel´o et al, 10.1103/Phys- RevD.83.041501, to analyse Hawking radiation in a Schwarzschild black hole as per- ceived by different observers in the system. -
Effect of Quantum Gravity on the Stability of Black Holes
S S symmetry Article Effect of Quantum Gravity on the Stability of Black Holes Riasat Ali 1 , Kazuharu Bamba 2,* and Syed Asif Ali Shah 1 1 Department of Mathematics, GC University Faisalabad Layyah Campus, Layyah 31200, Pakistan; [email protected] (R.A.); [email protected] (S.A.A.S.) 2 Division of Human Support System, Faculty of Symbiotic Systems Science, Fukushima University, Fukushima 960-1296, Japan * Correspondence: [email protected] Received: 10 April 2019; Accepted: 26 April 2019; Published: 5 May 2019 Abstract: We investigate the massive vector field equation with the WKB approximation. The tunneling mechanism of charged bosons from the gauged super-gravity black hole is observed. It is shown that the appropriate radiation consistent with black holes can be obtained in general under the condition that back reaction of the emitted charged particle with self-gravitational interaction is neglected. The computed temperatures are dependant on the geometry of black hole and quantum gravity. We also explore the corrections to the charged bosons by analyzing tunneling probability, the emission radiation by taking quantum gravity into consideration and the conservation of charge and energy. Furthermore, we study the quantum gravity effect on radiation and discuss the instability and stability of black hole. Keywords: higher dimension gauged super-gravity black hole; quantum gravity; quantum tunneling phenomenon; Hawking radiation 1. Introduction General relativity is associated with the thermodynamics and quantum effect which are strongly supportive of each other. A black hole (BH) is a compact object whose gravitational pull is so intense that can not escape the light. -
Field Theory Aspects of Cosmology and Black Holes
FIELD THEORY ASPECTS OF COSMOLOGY AND BLACK HOLES Thesis submitted for the degree of Doctor of Philosophy (Science) of Jadavpur University, Kolkata August 2009 arXiv:1011.6570v1 [hep-th] 30 Nov 2010 Kulkarni Shailesh Gajanan Satyendra Nath Bose National Centre for Basic Sciences JD Block, Sector 3, Salt Lake, Kolkata 700098, India Certificate from the supervisor This is to certify that the thesis entitled \Field theory aspects of cosmology and black holes" submitted by Sri. Kulkarni Shailesh Gajanan, who got his name registered on October 8, 2007 for the award of Ph.D. (Science) degree of Jadavpur University, is absolutely based upon his own work under the supervision of Professor Rabin Banerjee at S.N. Bose National Centre for Basic Sciences, Kolkata, India, and that neither this thesis nor any part of it has been submitted for any degree/diploma or any other academic award anywhere before. Rabin Banerjee Professor S.N. Bose National Centre for Basic Sciences JD Block, Sector 3, Salt Lake Kolkata 700098, India TO MY MOT HER Acknowledgements This thesis is the culminative outcome of five years work, which has been made possible by the blessings and support of many individuals. I take this opportunity to express my sincere gratitude to all of them. First and foremost, I would like to thank Prof. Rabin Banerjee, my thesis supervisor. His uncanny ability to select a particular problem, a keen and strategic analysis of it and deep involvement among the students makes him something special. Thank you Sir for giving me all that could last my entire life. -
Firewalls and the Quantum Properties of Black Holes
Firewalls and the Quantum Properties of Black Holes A thesis submitted in partial fulfillment of the requirements for the degree of Bachelor of Science degree in Physics from the College of William and Mary by Dylan Louis Veyrat Advisor: Marc Sher Senior Research Coordinator: Gina Hoatson Date: May 10, 2015 1 Abstract With the proposal of black hole complementarity as a solution to the information paradox resulting from the existence of black holes, a new problem has become apparent. Complementarity requires a vio- lation of monogamy of entanglement that can be avoided in one of two ways: a violation of Einstein’s equivalence principle, or a reworking of Quantum Field Theory [1]. The existence of a barrier of high-energy quanta - or “firewall” - at the event horizon is the first of these two resolutions, and this paper aims to discuss it, for Schwarzschild as well as Kerr and Reissner-Nordstr¨omblack holes, and to compare it to alternate proposals. 1 Introduction, Hawking Radiation While black holes continue to present problems for the physical theories of today, quite a few steps have been made in the direction of understanding the physics describing them, and, consequently, in the direction of a consistent theory of quantum gravity. Two of the most central concepts in the effort to understand black holes are the black hole information paradox and the existence of Hawking radiation [2]. Perhaps the most apparent result of black holes (which are a consequence of general relativity) that disagrees with quantum principles is the possibility of information loss. Since the only possible direction in which to pass through the event horizon is in, toward the singularity, it would seem that information 2 entering a black hole could never be retrieved. -
Arxiv:1410.1486V2 [Gr-Qc] 26 Aug 2015
October 2014 Black Hole Thermodynamics S. Carlip∗ Department of Physics University of California Davis, CA 95616 USA Abstract The discovery in the early 1970s that black holes radiate as black bodies has radically affected our understanding of general relativity, and offered us some early hints about the nature of quantum gravity. In this chapter I will review the discovery of black hole thermodynamics and summarize the many indepen- dent ways of obtaining the thermodynamic and (perhaps) statistical mechanical properties of black holes. I will then describe some of the remaining puzzles, including the nature of the quantum microstates, the problem of universality, and the information loss paradox. arXiv:1410.1486v2 [gr-qc] 26 Aug 2015 ∗email: [email protected] 1 Introduction The surprising discovery that black holes behave as thermodynamic objects has radically affected our understanding of general relativity and its relationship to quantum field theory. In the early 1970s, Bekenstein [1, 2] and Hawking [3, 4] showed that black holes radiate as black bodies, with characteristic temperatures and entropies ~κ Ahor kTH = ;SBH = ; (1.1) 2π 4~G where κ is the surface gravity and Ahor is the area of the horizon. These quantities appear to be inherently quantum gravitational, in the sense that they depend on both Planck's constant ~ and Newton's constant G. The resulting black body radiation, Hawking radiation, has not yet been directly observed: the temperature of an astrophysical black hole is on the order of a microkelvin, far lower than the cosmic microwave background temperature. But the Hawking temperature and the Bekenstein-Hawking entropy have been derived in so many independent ways, in different settings and with different assumptions, that it seems extraordinarily unlikely that they are not real. -
BLACK HOLE THERMODYNAMICS the Horizon Area Theorem 1970: Stephen Hawking Uses the Theory of General Relativity to Derive the So-Called
BLACK HOLE THERMODYNAMICS The horizon area theorem 1970: Stephen Hawking uses the theory of general relativity to derive the so-called Horizon area theorem The total horizon area in a closed system containing black holes never decreases. It can only increase or stay the same. [Stephen Hawking] Analogy between the area theorem and the 2nd law of thermodynamic Shortly after Stephen Hawking Formulated the area theorem, Jacob Beckenstein, at the time a graduate student at Princeton, noticed the analogy between the area theorem and the 2nd law of thermodynamics: [Jacob Beckenstein] The total area of a closed system never decreases. Entropy: logarithm of the number of ways you can relocate the atoms and molecules of a system without changing the overall properties of the system. Example of entropy: toys in a playroom (Thorne, pg. 424) Extremely orderly: 20 toys on 1 tile This playroom floor has 100 tiles, on which the kids can arrange 20 different toys. Parents prefer the toys to be kept in an extremely orderly configuration, with all the toys piled on one tile in one corner, as shown. There is only one such arrangement; the entropy of this configuration is thus the Number of equivalent rearrangements = 1; logarithm of 1, which is zero. entropy = 0. [This and next two slides courtesy of D. Watson] Entropy in a playroom (continued) Orderly: 20 toys on 10 tiles Parents might even accept this somewhat less orderly configuration: 20 different toys on 10 specific tiles. But there are lots of different equivalent arrangements (e.g. swapping the positions of two toys on different tiles produces a different arrangement that’s still acceptable): 1020 of them, in Number of equivalent rearrangements = 1020; fact, for an entropy value of “entropy” = 20. -
Quantum Wave Mechanics 3Rd Ed
Geometrical description of photons, electrons and composite particles. Dimensional analysis of electrical charge. Quantum gravity, gravitational frequency spectrum, mass oscillator synchronization, spectral energy density modulation and phase conjugation. Origin of charge, fine structure constant and inertia. Prospects for wave-based EM propulsion. Quantum Wave Mechanics by Larry Reed Order the complete book from the publisher Booklocker.com https://www.booklocker.com/p/books/10176.html?s=pdf or from your favorite neighborhood or online bookstore. To my parents who never knew the result of their great experiment Copyright © 2019, 2020 by Larry J. Reed All rights reserved. No part of this publication may be reproduced, stored in a retrieval system, or transmitted in any form or by any means, electronic, mechanical, recording or otherwise, without the prior written permission of the author. Printed on acid-free paper. Library of Congress Control Number: 2018901065 ISBN: 978-1-63492-964-6 paperback To order additional copies of this book, contact: www.booklocker.com CONTENTS Preface ........................................................................................................................... ix SECTION 1 – LIGHT 1. Photon model ................................................................................................................. 1 2. Quantum vacuum ......................................................................................................... 13 3. Electromagnetic 4-Potential ....................................................................................... -
Black Hole Thermodynamics
Black Hole Thermodynamics Reading: Wald 12.5 There is good evidence that after formation black holes relax to stationary configurations, characterized by mass, angular momentum, and gauge charges. This is a negligible amount of data compared to the many ways we can form black holes, suggesting that they ought to be thought of as thermodynamic entities. If so we need to identify their temperature and entropy and ask if they satisfy the laws of thermodynamics. This was a great discovery by Bekenstein and Hawking who showed black holes are thermal only after quantum effects are taken into account and their entropy is the horizon area=4G. To motivate these answers, let us return to the Kerr solution and consider the area of a constant t section of the horizon. The induced metric is (r2 + a2)2 ds2 = Σdθ2 + + sin2 θ d'2; (1) Σ and the resulting area is 2 2 2 2 p 4 4 2 2 A = 4π(r+ + a ) = 8π(G M + G M − G J ): (2) In the last step we used J = Ma and the definition of r+ to write A in terms of black hole mass and spin. Under an infinitesimal change dM and dJ, we obtaind p G4M 4 − G2J 2 dM = Ω dJ + dA: (3) H 2G2MA This equation is reminding of the first law of thermodynamics dE = µdQ + T dS (in a system with rotation symmetry, Ω is the chemical potential associated to the conserved charge J). It suggests identifying the horizon area with black hole entropy SBH / A; (4) though we need a different calculation to determine the temperature and hence the (positive) proportionality constant. -
Black Hole Radiation and Volume Statistical Entropy
Black Hole Radiation and Volume Statistical Entropy Mario Rabinowitz1 ________________________________________________________________________ G The simplest possible equation for Hawking radiation P = h , and other black SH 90 hole radiated power is derived in terms of black hole density, . Black hole density also leads to the simplest possible model of a gas of elementary constituents confined inside a gravitational bottle of Schwarzchild radius at tremendous pressure, which yields identically the same functional dependence 3 as the traditional black hole entropy S bh ()kAc / hG . Variations of Sbh can be obtained which depend on the occupancy of phase space cells. A relation is R derived between the constituent momenta and the black hole radius H , 3 h p = , which is similar to the Compton wavelength relation. 2 R H ________________________________________________________________________ Key Words: Black Hole Entropy, Hawking Radiation, Black Hole density. 1. INTRODUCTION The object of this paper is to gain an insight into black holes. This is first done by finding the simplest possible equation for black hole radiation. Then we shall find the simplest possible model which can give some comprehension as to why black hole entropy appears to be related only to its surface area. This attempt at understanding black hole entropy is done in the same spirit as was the paper on Classical Tunneling (Cohn and Rabinowitz, 1990) which showed how far a simple classical model can go to illume the phenomenon of quantum tunneling . 1Armor Research, 715 Lakemead Way; Redwood City, California 94062-3922 -1- of 10 The strategy here will be to find the number of elementary constituents, N, which fill a black hole, simply modeled as a gravitational bottle. -
Arxiv:1905.01301V1 [Hep-Ph] 3 May 2019 Radiation and Dark Matter [77, 80, 84]
FERMILAB-PUB-19-186-A Dark Radiation and Superheavy Dark Matter from Black Hole Domination Dan Hoopera;b;c,∗ Gordan Krnjaica,y and Samuel D. McDermottaz aFermi National Accelerator Laboratory, Theoretical Astrophysics Group, Batavia, IL 60510 bUniversity of Chicago, Kavli Institute for Cosmological Physics, Chicago, IL 60637 and cUniversity of Chicago, Department of Astronomy and Astrophysics, Chicago, IL 60637 (Dated: May 6, 2019) If even a relatively small number of black holes were created in the early universe, they will constitute an increasingly large fraction of the total energy density as space expands. It is thus well-motivated to consider scenarios in which the early universe included an era in which primordial black holes dominated the total energy density. Within this context, we consider Hawking radiation as a mechanism to produce both dark radiation and dark matter. If the early universe included a black hole dominated era, we find that Hawking radiation will produce dark radiation at a level ∆Neff 0:03 0:2 for each light and decoupled species of spin 0, 1/2, or 1. This range is well suited∼ to relax− the tension between late and early-time Hubble determinations, and is within the reach of upcoming CMB experiments. The dark matter could also originate as Hawking radiation in a black hole dominated early universe, although such dark matter candidates must be very heavy 11 (mDM > 10 GeV) if they are to avoid exceeding the measured abundance. ∼ I. INTRODUCTION It has long been appreciated that inhomogeneties in the early universe could lead to the formation of primordial black holes [1].