Astrophysical Hints for Magnetic Black Holes
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Exploring Black Holes As Particle Accelerators in Realistic Scenarios
Exploring black holes as particle accelerators in realistic scenarios Stefano Liberati∗ SISSA, Via Bonomea 265, 34136 Trieste, Italy and INFN, Sezione di Trieste; IFPU - Institute for Fundamental Physics of the Universe, Via Beirut 2, 34014 Trieste, Italy Christian Pfeifer† ZARM, University of Bremen, 28359 Bremen, Germany José Javier Relancio‡ Dipartimento di Fisica “Ettore Pancini”, Università di Napoli Federico II, Napoli, Italy; INFN, Sezione di Napoli, Italy; Centro de Astropartículas y Física de Altas Energías (CAPA), Universidad de Zaragoza, Zaragoza 50009, Spain The possibility that rotating black holes could be natural particle accelerators has been subject of intense debate. While it appears that for extremal Kerr black holes arbitrarily high center of mass energies could be achieved, several works pointed out that both theoretical as well as astrophysical arguments would severely dampen the attainable energies. In this work we study particle collisions near Kerr–Newman black holes, by reviewing and extending previously proposed scenarios. Most importantly, we implement the hoop conjecture for all cases and we discuss the astrophysical relevance of these collisional Penrose processes. The outcome of this investigation is that scenarios involving near-horizon target particles are in principle able to attain, sub-Planckian, but still ultra high, center of mass energies of the order of 1021 −1023 eV. Thus, these target particle collisional Penrose processes could contribute to the observed spectrum of ultra high-energy cosmic rays, even if the hoop conjecture is taken into account, and as such deserve further scrutiny in realistic settings. I. INTRODUCTION Since Penrose’s original paper [1], pointing out the possibility to exploit rotating black holes’ ergoregions to extract energy, there have been several efforts in the literature aiming at developing and optimizing this idea. -
Disrupting Entanglement of Black Holes Arxiv:1405.7365V2 [Hep-Th] 23 Jun 2014
CALT-TH-2014-139 Disrupting Entanglement of Black Holes Stefan Leichenauer Walter Burke Institute for Theoretical Physics California Institute of Technology, Pasadena, CA 91125 Abstract We study entanglement in thermofield double states of strongly coupled CFTs by analyzing two-sided Reissner-Nordstr¨omsolutions in AdS. The central object of study is the mutual information between a pair of regions, one on each asymptotic boundary of the black hole. For large regions the mutual information is positive and for small ones it vanishes; we compute the critical length scale, which goes to infinity for extremal black holes, of the transition. We also generalize the butterfly effect of Shenker and Stanford [1] to a wide class of charged black holes, showing that mutual information is disrupted upon perturbing the system and waiting for a time of order log E/δE in units of the temperature. We conjecture that the parametric form of this timescale is universal. arXiv:1405.7365v2 [hep-th] 23 Jun 2014 email: [email protected] Contents 1 Introduction 3 2 The Setup 5 3 Temperature Dependence of Mutual Information 6 4 The Butterfly Effect 8 4.1 Shockwave Geometry . .8 4.2 Extremal Surfaces . 11 4.2.1 Surface Location . 12 4.2.2 Surface Area . 14 5 Discussion 15 A RNAdS Thermodynamics 16 B Exact Results in d = 4 17 C Near-Extremal Black Holes 18 2 1 Introduction The connection between geometry and entanglement is exciting and deep. In particular, the recent ER=EPR framework introduced by Maldacena and Susskind [2] suggests that, in a grav- itational theory, we should always associate entanglements with wormholes. -
Light Rays, Singularities, and All That
Light Rays, Singularities, and All That Edward Witten School of Natural Sciences, Institute for Advanced Study Einstein Drive, Princeton, NJ 08540 USA Abstract This article is an introduction to causal properties of General Relativity. Topics include the Raychaudhuri equation, singularity theorems of Penrose and Hawking, the black hole area theorem, topological censorship, and the Gao-Wald theorem. The article is based on lectures at the 2018 summer program Prospects in Theoretical Physics at the Institute for Advanced Study, and also at the 2020 New Zealand Mathematical Research Institute summer school in Nelson, New Zealand. Contents 1 Introduction 3 2 Causal Paths 4 3 Globally Hyperbolic Spacetimes 11 3.1 Definition . 11 3.2 Some Properties of Globally Hyperbolic Spacetimes . 15 3.3 More On Compactness . 18 3.4 Cauchy Horizons . 21 3.5 Causality Conditions . 23 3.6 Maximal Extensions . 24 4 Geodesics and Focal Points 25 4.1 The Riemannian Case . 25 4.2 Lorentz Signature Analog . 28 4.3 Raychaudhuri’s Equation . 31 4.4 Hawking’s Big Bang Singularity Theorem . 35 5 Null Geodesics and Penrose’s Theorem 37 5.1 Promptness . 37 5.2 Promptness And Focal Points . 40 5.3 More On The Boundary Of The Future . 46 1 5.4 The Null Raychaudhuri Equation . 47 5.5 Trapped Surfaces . 52 5.6 Penrose’s Theorem . 54 6 Black Holes 58 6.1 Cosmic Censorship . 58 6.2 The Black Hole Region . 60 6.3 The Horizon And Its Generators . 63 7 Some Additional Topics 66 7.1 Topological Censorship . 67 7.2 The Averaged Null Energy Condition . -
Plasma Modes in Surrounding Media of Black Holes and Vacuum Structure - Quantum Processes with Considerations of Spacetime Torque and Coriolis Forces
COLLECTIVE COHERENT OSCILLATION PLASMA MODES IN SURROUNDING MEDIA OF BLACK HOLES AND VACUUM STRUCTURE - QUANTUM PROCESSES WITH CONSIDERATIONS OF SPACETIME TORQUE AND CORIOLIS FORCES N. Haramein¶ and E.A. Rauscher§ ¶The Resonance Project Foundation, [email protected] §Tecnic Research Laboratory, 3500 S. Tomahawk Rd., Bldg. 188, Apache Junction, AZ 85219 USA Abstract. The main forces driving black holes, neutron stars, pulsars, quasars, and supernovae dynamics have certain commonality to the mechanisms of less tumultuous systems such as galaxies, stellar and planetary dynamics. They involve gravity, electromagnetic, and single and collective particle processes. We examine the collective coherent structures of plasma and their interactions with the vacuum. In this paper we present a balance equation and, in particular, the balance between extremely collapsing gravitational systems and their surrounding energetic plasma media. Of particular interest is the dynamics of the plasma media, the structure of the vacuum, and the coupling of electromagnetic and gravitational forces with the inclusion of torque and Coriolis phenomena as described by the Haramein-Rauscher solution to Einstein’s field equations. The exotic nature of complex black holes involves not only the black hole itself but the surrounding plasma media. The main forces involved are intense gravitational collapsing forces, powerful electromagnetic fields, charge, and spin angular momentum. We find soliton or magneto-acoustic plasma solutions to the relativistic Vlasov equations solved in the vicinity of black hole ergospheres. Collective phonon or plasmon states of plasma fields are given. We utilize the Hamiltonian formalism to describe the collective states of matter and the dynamic processes within plasma allowing us to deduce a possible polarized vacuum structure and a unified physics. -
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. -
Jhep02(2019)160
Published for SISSA by Springer Received: January 18, 2019 Accepted: February 10, 2019 Published: February 25, 2019 Holographic complexity equals which action? JHEP02(2019)160 Kanato Goto,a Hugo Marrochio,b;c Robert C. Myers,b Leonel Queimadab;c and Beni Yoshidab aThe University of Tokyo, Komaba, Meguro-ku, Tokyo 153-8902, Japan bPerimeter Institute for Theoretical Physics, Waterloo, ON N2L 2Y5, Canada cDepartment of Physics & Astronomy, University of Waterloo, Waterloo, ON N2L 3G1, Canada E-mail: [email protected], [email protected], [email protected], [email protected], [email protected] Abstract: We revisit the complexity = action proposal for charged black holes. We in- vestigate the complexity for a dyonic black hole, and we find the surprising feature that the late-time growth is sensitive to the ratio between electric and magnetic charges. In particular, the late-time growth rate vanishes when the black hole carries only a magnetic charge. If the dyonic black hole is perturbed by a light shock wave, a similar feature ap- pears for the switchback effect, e.g. it is absent for purely magnetic black holes. We then show how the inclusion of a surface term to the action can put the electric and magnetic charges on an equal footing, or more generally change the value of the late-time growth rate. Next, we investigate how the causal structure influences the late-time growth with and without the surface term for charged black holes in a family of Einstein-Maxwell-Dilaton theories. Finally, we connect the previous discussion to the complexity=action proposal for the two-dimensional Jackiw-Teitelboim theory. -
SAM Lectures on Extremal Black Holes in D = 4 Extended Supergravity Stefano Bellucci♣, Sergio Ferrara♦♣[, Murat G¨Unaydin♠ and Alessio Marrani♥
CERN-PH-TH/2009-070 UCLA/09/TEP/51 SU-ITP-09/19 SAM Lectures on Extremal Black Holes in d = 4 Extended Supergravity Stefano Bellucci|, Sergio Ferrara}|[, Murat G¨unaydin♠ and Alessio Marrani~ | INFN - Laboratori Nazionali di Frascati, Via Enrico Fermi 40,00044 Frascati, Italy [email protected] } Physics Department,Theory Unit, CERN, CH 1211, Geneva 23, Switzerland [email protected] [ Department of Physics and Astronomy, University of California, Los Angeles, CA USA ♠ Department of Physics, Penn State University University Park, PA16802, USA [email protected] ~ Stanford Institute for Theoretical Physics Department of Physics, 382 Via Pueblo Mall, Varian Lab, Stanford University, Stanford, CA 94305-4060, USA [email protected] Contribution to the Proceedings of the School on Attractor Mechanism 2007 (SAM2007), June 18{22 2007, INFN{LNF, Frascati, Italy Abstract We report on recent results in the study of extremal black hole attractors in N = 2, arXiv:0905.3739v1 [hep-th] 22 May 2009 d = 4 ungauged Maxwell-Einstein supergravities. For homogeneous symmetric scalar manifolds, the three general classes of attractor so- lutions with non-vanishing Bekenstein-Hawking entropy are discussed. They correspond to three (inequivalent) classes of orbits of the charge vector, which sits in the relevant sym- 1 plectic representation RV of the U-duality group. Other than the 2 -BPS one, there are two other distinct non-BPS classes of charge orbits, one of which has vanishing central charge. The complete classification of the U-duality orbits, as well as of the moduli spaces of non-BPS attractors (spanned by the scalars which are not stabilized at the black hole event horizon), is also reviewed. -
Black Holes and String Theory
Black Holes and String Theory Hussain Ali Termezy Submitted in partial fulfilment of the requirements for the degree of Master of Science of Imperial College London September 2012 Contents 1 Black Holes in General Relativity 2 1.1 Black Hole Solutions . 2 1.2 Black Hole Thermodynamics . 5 2 String Theory Background 19 2.1 Strings . 19 2.2 Supergravity . 23 3 Type IIB and Dp-brane solutions 25 4 Black Holes in String Theory 33 4.1 Entropy Counting . 33 Introduction The study of black holes has been an intense area of research for many decades now, as they are a very useful theoretical construct where theories of quantum gravity become relevant. There are many curiosities associated with black holes, and the resolution of some of the more pertinent problems seem to require a quantum theory of gravity to resolve. With the advent of string theory, which purports to be a unified quantum theory of gravity, attention has naturally turned to these questions, and have remarkably shown signs of progress. In this project we will first review black hole solutions in GR, and then look at how a thermodynamic description of black holes is made possible. We then turn to introduce string theory and in particular review the black Dp-brane solutions of type IIB supergravity. Lastly we see how to compute a microscopic account of the Bekenstein entropy is given in string theory. 1 Chapter 1 Black Holes in General Relativity 1.1 Black Hole Solutions We begin by reviewing some the basics of black holes as they arise in the study of general relativity. -
On the Distribution of Stellar-Sized Black Hole Spins
11th Edoardo Amaldi Conference on Gravitational Waves (AMALDI 11) IOP Publishing Journal of Physics: Conference Series 716 (2016) 012002 doi:10.1088/1742-6596/716/1/012002 On the distribution of stellar-sized black hole spins Alex B. Nielsen Max Planck Institut f¨urGravitationsphysik, Callinstrasse 38, D-30167 Hannover, Germany and Leibniz Universit¨at Hannover, Welfengarten 1-A, D-30167 Hannover, Germany Abstract. Black hole spin will have a large impact on searches for gravitational waves with advanced detectors. While only a few stellar mass black hole spins have been measured using X- ray techniques, gravitational wave detectors have the capacity to greatly increase the statistics of black hole spin measurements. We show what we might learn from these measurements and how the black hole spin values are influenced by their formation channels. 1. Introduction Gravitational wave observations will be sensitive to the spins of black holes [3]. Simulated search pipelines indicate that accounting for black hole spin can substantially improve the sensitivity of gravitational wave searches for binaries containing one [2] or two [15] black holes. However, this improvement comes at a cost of increased computational resources and is only realised if the spins of black holes are indeed significant. It is therefore necessary to balance the increased cost with the expectation that black holes will indeed have large spins. Here we discuss that evidence. 2 Truly isolated black holes are expected to satisfy the Kerr bound, a∗ ≡ cJ=GM < 1, where J and M denote the angular momentum and mass of the black hole and c and G the speed of light and Newton's gravitational constant respectively. -
The Collisional Penrose Process
Noname manuscript No. (will be inserted by the editor) The Collisional Penrose Process Jeremy D. Schnittman Received: date / Accepted: date Abstract Shortly after the discovery of the Kerr metric in 1963, it was realized that a region existed outside of the black hole's event horizon where no time-like observer could remain stationary. In 1969, Roger Penrose showed that particles within this ergosphere region could possess negative energy, as measured by an observer at infinity. When captured by the horizon, these negative energy parti- cles essentially extract mass and angular momentum from the black hole. While the decay of a single particle within the ergosphere is not a particularly efficient means of energy extraction, the collision of multiple particles can reach arbitrar- ily high center-of-mass energy in the limit of extremal black hole spin. The re- sulting particles can escape with high efficiency, potentially erving as a probe of high-energy particle physics as well as general relativity. In this paper, we briefly review the history of the field and highlight a specific astrophysical application of the collisional Penrose process: the potential to enhance annihilation of dark matter particles in the vicinity of a supermassive black hole. Keywords black holes · ergosphere · Kerr metric 1 Introduction We begin with a brief overview of the Kerr metric for spinning, stationary black holes [1]. By far the most convenient, and thus most common form of the Kerr metric is the form derived by Boyer and Lindquist [2]. In standard spherical coor- -
Conformal Field Theory and Black Hole Physics
CONFORMAL FIELD THEORY AND BLACK HOLE PHYSICS Steve Sidhu Bachelor of Science, University of Northern British Columbia, 2009 A Thesis Submitted to the School of Graduate Studies of the University of Lethbridge in Partial Fulfilment of the Requirements for the Degree MASTER OF SCIENCE Department of Physics and Astronomy University of Lethbridge LETHBRIDGE, ALBERTA, CANADA c Steve Sidhu, 2012 Dedication To my parents, my sister, and Paige R. Ryan. iii Abstract This thesis reviews the use of 2-dimensional conformal field theory applied to gravity, specifically calculating Bekenstein-Hawking entropy of black holes in (2+1) dimen- sions. A brief review of general relativity, Conformal Field Theory, energy extraction from black holes, and black hole thermodynamics will be given. The Cardy formula, which calculates the entropy of a black hole from the AdS/CFT duality, will be shown to calculate the correct Bekenstein-Hawking entropy of the static and rotating BTZ black holes. The first law of black hole thermodynamics of the static, rotating, and charged-rotating BTZ black holes will be verified. iv Acknowledgements I would like to thank my supervisors Mark Walton and Saurya Das. I would also like to thank Ali Nassar and Ahmed Farag Ali for the many discussions, the Theo- retical Physics Group, and the entire Department of Physics and Astronomy at the University of Lethbridge. v Table of Contents Approval/Signature Page ii Dedication iii Abstract iv Acknowledgements v Table of Contents vi 1 Introduction 1 2 Einstein’s field equations and black hole solutions 7 2.1 Conventions and notations . 7 2.2 Einstein’s field equations . -
Semiclassical Decay of Near-Extremal Black Holes
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server UMDGR-97-110 hep-th/9705017 Semiclassical Decay of Near-Extremal Black Holes Ted Jacobson Department of Physics, University of Maryland College Park, MD 20742-4111, USA [email protected] Abstract Decay of a near-extremal black hole down to the extremal state is studied in the background field approximation to determine the fate of injected matter and Hawking pairs. By examining the behavior of light rays and solutions to the wave equation it is concluded that the singularity at the origin is irrelevant. Furthermore, there is most likely an instability of the event horizon arising from the accumulation of injected matter and Hawking partners there. The possible role of this instability in reconciling the D-brane and black hole pictures of the decay process is discussed. 1 Introduction The decay of black holes by quantum emission of thermal radiation suggests that quantum gravity is not unitary[1]. Two types of information appear to be lost in the decay process, the state of the matter that falls into the black hole and the correlations between the Hawking quanta that are radiated away and their “partners” in the pair creation process. If the black hole evaporates completely this information seems to be destroyed, at least as far as the outside observer is concerned. The argument that quantum gravity is not unitary is of course inconclusive at present since we lack a complete theory. According to one point of view the unitarity question hinges on the physics of the curvature singularity inside the black hole.