DOCSLIB.ORG

Black Holes of N=8 Supergravity

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Black Holes of N=8 Supergravity Black holes of = 8 supergravity N Geoffrey Compère Université Libre de Bruxelles (ULB) Ascona, July 2014 G. Compère (ULB) 1 / 35 The simplicity of = 8 supergravity N Obtained as the low energy regime of M-theory upon compactification on T7 Inherits E7(7)(R) symmetries broken to E7(7)(Z) at the quantum level Cremmer and Julia (1978), etc In perturbation theory, UV finite up to 4, maybe 8, loops Bern et al. (2009), etc In perturbation theory, amplitudes enjoy remarkable properties : square of N = 4 SYM, etc Kawai, Lewellen, Tye (1986), etc The theory cannot be decoupled from string theory Green, Ooguri, Schwarz (2007) The theory contains BPS extremal black holes with known microscopic counting in M-theory Maldacena, Strominger, Witten (1997). G. Compère (ULB) 2 / 35 Ideal setup to address black hole microscopics All known non-extremal black holes in string theory obey Cvetič and Larsen (1997) 2 S+S− π Z 2 All known extremal black holes have SL(2; R) U(1) × SL(2; R) Virasoro symmetries and obey ! × π2 π2 S = c T = c T + 3 J J 3 Q Q Are there other “IR” universal formulae ? Is there a proof from the “UV" ? In this talk, I will present the most general asymptotically flat non-extremal black hole of = 8 supergravity and N derive some of its properties. G. Compère (ULB) 3 / 35 (Next to simple) Gauged = 8 SO(8) supergravity N Obtained as the low energy regime of M-theory upon compactification on S7 Admits AdS as a = 8 vacuum 4 N When embedded in M-theory, the dual CFT is the ABJM theory at level k = 1. Aharony, Bergman, Jafferis, Maldacena (2008) New sugra theories labelled by a continuous parameter have been recently found Dall’Agata, Inverso, Trigiante (2012) Much less is known on solutions and “IR" relations Known black holes in AdS4 obey Cvetič, Gibbons, Pope (2010) 4 4 S+ S− Si S−i π ` Z 2 In this talk, I will present some black holes of this theory and discuss subtleties with their thermodynamics G. Compère (ULB) 4 / 35 Based on work done with David Chow (ULB) “Seed for general rotating non-extremal black holes of = 8 supergravity”, arXiv :1310.1925 N “Dyonic AdS black holes in maximal gauged supergravity”, arXiv :1311.1204 “Black holes in = 8 supergravity from SO(4; 4) hidden N symmetries”, arXiv :1404.2602 G. Compère (ULB) 5 / 35 Outline 1 STU supergravity and hidden symmetries 2 The general black hole and its properties 3 Microscopic counting for extremal branches 4 Dyonic black holes of maximal gauged supergravity G. Compère (ULB) 6 / 35 I. STU supergravity and hidden symmetries G. Compère (ULB) 7 / 35 From = 8 to STU supergravity N Under U-dualities, the 4d metric will be unchanged. The matter field will be shuffled around. There are 28 abelian gauge fields in = 8 supergravity. If N one starts with a dyonic rotating black hole with 3 additional electric charges (5 charges in total), one can perform U-dualities and generate the general black hole. Cvetič-Hull, 1996 A suitable sector of = 8 supergravity is a = 2 N N supergravity with three vector multiplets known as the STU supergravity Cremmer et al ’85 ; Duff et al. ’96. This is the theory that we will study here. G. Compère (ULB) 8 / 35 STU supergravity In a specific U-duality frame the Lagrangian has the general form Duff et al. ’96 1 = d4xp g R f (z)@ zA@µzB L4 − − 2 AB µ 1 1 k (z)FI FJµν + h (z)µνρσFI FJ −4 IJ µν 4 IJ µν ρσ where zj = xj + i yj, j = 1; 2; 3 are three complex scalar fields AI = (A1; A2; A3; A4) are the four U(1) gauge fields. Triality symmetry : SL(2; R) SL(2; R) SL(2; R) and their × × permutations. G. Compère (ULB) 9 / 35 From = 8 to STU supergravity N =8 N supergravity U-duality STU supergravity A2 = A3 ST2 supergravity (reduction of 6d minimal supergravity) A2 = A3 = A4 A1 = A4,A2 = A3 S3 supergravity iX0X1 supergravity − (reduction of 5d (truncation of minimal supergravity) = 4 supergravity) N A2 = A3 = A4 =0 AI = A A1 = A4,A2 = A3 =0 Einstein– Einstein–Maxwell– Kaluza–Klein theory Maxwell theory dilaton–axion theory ( = 2 supergravity) N G. Compère (ULB) 10 / 35 1 Known solutions =8 N supergravity U-duality Extremal Rotating 4-electric STU supergravity Static Rotating 4-dyonic A2 = A3 ST2 supergravity (reduction of 6d minimal supergravity) A2 = A3 = A4 A1 = A4,A2 = A3 S3 supergravity iX0X1 supergravity − (reduction of 5d (truncation of minimal supergravity) = 4 supergravity) N A2 = A3 = A4 =0 AI = A A1 = A4,A2 = A3 =0 Einstein– Einstein–Maxwell– Kaluza–Klein theory Maxwell theory dilaton–axion theory ( = 2 supergravity) N G. Compère (ULB) 11 / 35 1 Algorithm for solution generation Reduce on time. Get Euclidean 3d Einstein gravity coupled to scalars. SO(4;4) Scalars form the coset model Breitenlohner, Maison, Gibbons, ’88 SL(2;R)4 Take Kerr-Taub-NUT (a; m; n) as a seed Act with SL(2; R)4 SO(4; 4) hidden symmetries ⊂ I Generate all 4 QI + 4 P charges Cancel the total NUT charge at the end by tuning the initial NUT charge n Iterate the loop "Recognize patterns Simplify ! ! Rewrite Recognize patterns . ." ! ! G. Compère (ULB) 12 / 35 II. The general black hole and its properties G. Compère (ULB) 13 / 35 The Kerr metric (1963) R U dr2 du2 RU ds2 = − (dt + ! )2 + W + + dφ2 ; − W 3 R U a2(R U) − where W(r; u) = r2 + u2; 2mrU ! (r; u) = dφ, 3 a(R U) − and R(r) = r2 2mr + a2; − U(u) = a2 u2; − The standard spherical polar angle θ is u = a cos θ. G. Compère (ULB) 14 / 35 The = 8 black hole metric N Input : M; N; m; n; a + 2 harmonic functions L(r), V(u) : R U dr2 du2 RU ds2 = − (dt + ! )2 + W + + dφ2 ; − W 3 R U a2(R U) − where W2(r; u) = (R U)2 + (2Nu + L)2 + 2(R U)(2Mr + V) ; − − 2N(u n)R + U(L + 2Nn) ! (r; u) = − dφ, 3 a(R U) − R(r) = r2 2mr + a2 n2; − − U(u) = a2 (u n)2; − − L(r) = L1r + L2; V(u) = V1u + V2: The standard spherical polar angle θ is u = n + a cos θ. G. Compère (ULB) 15 / 35 Separability and hidden conformal symmetry Define the string frame metric 2 r2 + u2 ds~ = ds2: W It admits an irreducible Killing-Stäckel tensor Kab obeying K = 0: r(a bc) 2 The massive Klein-Gordon equation on ds~ is separable. Therefore, the metric ds2 admits an irreducible conformal Killing-Stäckel tensor with components Qab = Kab obeying Q = q g : r(a bc) (a bc) The massless Klein-Gordon equation on ds2 is separable. [Subcases include : Chow, ’08 ; Keeler, Larsen, ’12] G. Compère (ULB) 16 / 35 Gauge fields : All is known ! We have I @ 1 A = W (dt + !3) : @δI −W The electric and magnetic charges are @M I @N QI = 2 ; P = 2 : @δI − @δI G. Compère (ULB) 17 / 35 Scalar fields The three axions and dilatons are : f W i e−'i χi = 2 2 ; = 2 2 ; r + u + gi r + u + gi where f (r; u) = 2(mr + nu)ξ + 2(mu nr)ξ + 4(m2 + n2)ξ ; i i1 − i2 i3 g (r; u) = 2(mr + nu)η + 2(mu nr)η + 4(m2 + n2)η ; i i1 − i2 i3 are linear functions of r and u. G. Compère (ULB) 18 / 35 Thermodynamics First law and Smarr relation hold I + I δM = T+δS+ + Ω+δJ + Φ+δQI + ΨI δP ; I + I M = 2T+S+ + 2Ω+J + Φ+QI + ΨI P ; Also at the inner horizon, I − I δM = T−δS− + Ω−δJ + Φ−δQI + ΨI δP ; I − I M = 2T−S− + 2Ω−J + Φ−QI + ΨI P : G. Compère (ULB) 19 / 35 Quartic invariant 1 1 2 3 4 ∆ = 16 [4(Q1Q2Q3Q4 + P P P P ) + 2 P Q Q PJPK P (Q )2(PJ)2]: J<K J K − J J The invariant is a Cayley hyperdeterminant, and is manifestly 3 invariant under SL(2; R) upon rewriting as [Duff, ’06] 1 ii0 jj0 kk0 ll0 mm0 nn0 ∆ = 32 aijkai0j0manpk0 an0p0m0 ij [ij] 01 with = , = 1 and components aijk given by (a ; a ) = (Q ; P1); (a ; a ) = (P2; Q ); 000 111 − 1 001 110 2 3 4 (a010; a101) = (P ; Q3); (a011; a100) = (Q4; P ): This invariant is a special case of a more general E7(7) quartic invariant [Kallosh, Kol, ’96]. G. Compère (ULB) 20 / 35 Universal properties of horizons Product of area law : Cvetič, Gibbons, Pope, ’10 A+ A− 2 2 I 2 = 4π J + ∆(QI; P ) π Z 4 4 2 Angular momentum law : 2 Ω+ 2 8π J = (S+ S−) 4π Z T+ − 2 Kinematic relationship : Ω Ω− + = T+ − T− G. Compère (ULB) 21 / 35 A new E7(7)(R) invariant Using these properties, one can prove Cardy’s form : p q S = 2π ∆ + F + J2 + F + − I i Since S+; J; ∆ are E7(7)(R) invariants, then F(M; QI; P ; z1) is invariant as well. Known special cases : For BPS black holes, F = J = 0. In the extremal “fast” rotating limit, F = J2. In the extremal “slow” rotating limit, F = ∆ − For Kerr-Newman : F = M4 M2Q2. 1− In regime Q : F = Q Q Q (M M ) Cvetic-Larsen 1;2;3 ! 1 2 1 2 3 − BPS (2014) G. Compère (ULB) 22 / 35 F is not a rational function of the charges For the Kaluza-Klein black hole (Rasheed-Larsen), 1 1 1 1 F = (M2 P2)(M2 Q2) + (M2 + (P2 + Q2))2H[x] − 4 − 4 3 8 2 2 2 2 where 0 x 54M (P −Q ) 1 and ≤ ≡ (8M2+P2+Q2)3 ≤ p arcsin px arcsin px H[x] = 2 1 x cos + 6px sin 2 − 3 3 − increases monotonically from 0 to 1.
Load more

Recommended publications
  • Limits on New Physics from Black Holes Arxiv:1309.0530V1
    Limits on New Physics from Black Holes Clifford Cheung and Stefan Leichenauer California Institute of Technology, Pasadena, CA 91125 Abstract Black holes emit high energy particles which induce a finite density potential for any scalar field φ coupling to the emitted quanta. Due to energetic considerations, φ evolves locally to minimize the effective masses of the outgoing states. In theories where φ resides at a metastable minimum, this effect can drive φ over its potential barrier and classically catalyze the decay of the vacuum. Because this is not a tunneling process, the decay rate is not exponentially suppressed and a single black hole in our past light cone may be sufficient to activate the decay. Moreover, decaying black holes radiate at ever higher temperatures, so they eventually probe the full spectrum of particles coupling to φ. We present a detailed analysis of vacuum decay catalyzed by a single particle, as well as by a black hole. The former is possible provided large couplings or a weak potential barrier. In contrast, the latter occurs much more easily and places new stringent limits on theories with hierarchical spectra. Finally, we comment on how these constraints apply to the standard model and its extensions, e.g. metastable supersymmetry breaking. arXiv:1309.0530v1 [hep-ph] 2 Sep 2013 1 Contents 1 Introduction3 2 Finite Density Potential4 2.1 Hawking Radiation Distribution . .4 2.2 Classical Derivation . .6 2.3 Quantum Derivation . .8 3 Catalyzed Vacuum Decay9 3.1 Scalar Potential . .9 3.2 Point Particle Instability . 10 3.3 Black Hole Instability . 11 3.3.1 Tadpole Instability .
    [Show full text]
  • Spacetime Geometry from Graviton Condensation: a New Perspective on Black Holes
    Spacetime Geometry from Graviton Condensation: A new Perspective on Black Holes Sophia Zielinski née Müller München 2015 Spacetime Geometry from Graviton Condensation: A new Perspective on Black Holes Sophia Zielinski née Müller Dissertation an der Fakultät für Physik der Ludwig–Maximilians–Universität München vorgelegt von Sophia Zielinski geb. Müller aus Stuttgart München, den 18. Dezember 2015 Erstgutachter: Prof. Dr. Stefan Hofmann Zweitgutachter: Prof. Dr. Georgi Dvali Tag der mündlichen Prüfung: 13. April 2016 Contents Zusammenfassung ix Abstract xi Introduction 1 Naturalness problems . .1 The hierarchy problem . .1 The strong CP problem . .2 The cosmological constant problem . .3 Problems of gravity ... .3 ... in the UV . .4 ... in the IR and in general . .5 Outline . .7 I The classical description of spacetime geometry 9 1 The problem of singularities 11 1.1 Singularities in GR vs. other gauge theories . 11 1.2 Defining spacetime singularities . 12 1.3 On the singularity theorems . 13 1.3.1 Energy conditions and the Raychaudhuri equation . 13 1.3.2 Causality conditions . 15 1.3.3 Initial and boundary conditions . 16 1.3.4 Outlining the proof of the Hawking-Penrose theorem . 16 1.3.5 Discussion on the Hawking-Penrose theorem . 17 1.4 Limitations of singularity forecasts . 17 2 Towards a quantum theoretical probing of classical black holes 19 2.1 Defining quantum mechanical singularities . 19 2.1.1 Checking for quantum mechanical singularities in an example spacetime . 21 2.2 Extending the singularity analysis to quantum field theory . 22 2.2.1 Schrödinger representation of quantum field theory . 23 2.2.2 Quantum field probes of black hole singularities .
    [Show full text]
  • Black Hole Production and Graviton Emission in Models with Large Extra Dimensions
    Black hole production and graviton emission in models with large extra dimensions Dissertation zur Erlangung des Doktorgrades der Naturwissenschaften vorgelegt beim Fachbereich Physik der Johann Wolfgang Goethe–Universit¨at in Frankfurt am Main von Benjamin Koch aus N¨ordlingen Frankfurt am Main 2007 (D 30) vom Fachbereich Physik der Johann Wolfgang Goethe–Universit¨at als Dissertation angenommen Dekan ........................................ Gutachter ........................................ Datum der Disputation ................................ ........ Zusammenfassung In dieser Arbeit wird die m¨ogliche Produktion von mikroskopisch kleinen Schwarzen L¨ochern und die Emission von Gravitationsstrahlung in Modellen mit großen Extra-Dimensionen untersucht. Zun¨achst werden der theoretisch-physikalische Hintergrund und die speziel- len Modelle des behandelten Themas skizziert. Anschließend wird auf die durchgefuhrten¨ Untersuchungen zur Erzeugung und zum Zerfall mikrosko- pisch kleiner Schwarzer L¨ocher in modernen Beschleunigerexperimenten ein- gegangen und die wichtigsten Ergebnisse zusammengefasst. Im Anschluss daran wird die Produktion von Gravitationsstrahlung durch Teilchenkollisio- nen diskutiert. Die daraus resultierenden analytischen Ergebnisse werden auf hochenergetische kosmische Strahlung angewandt. Die Suche nach einer einheitlichen Theorie der Naturkr¨afte Eines der großen Ziele der theoretischen Physik seit Einstein ist es, eine einheitliche und m¨oglichst einfache Theorie zu entwickeln, die alle bekannten Naturkr¨afte beschreibt.
    [Show full text]
  • Black Holes and Qubits
    Subnuclear Physics: Past, Present and Future Pontifical Academy of Sciences, Scripta Varia 119, Vatican City 2014 www.pas.va/content/dam/accademia/pdf/sv119/sv119-duff.pdf Black Holes and Qubits MICHAEL J. D UFF Blackett Labo ratory, Imperial C ollege London Abstract Quantum entanglement lies at the heart of quantum information theory, with applications to quantum computing, teleportation, cryptography and communication. In the apparently separate world of quantum gravity, the Hawking effect of radiating black holes has also occupied centre stage. Despite their apparent differences, it turns out that there is a correspondence between the two. Introduction Whenever two very different areas of theoretical physics are found to share the same mathematics, it frequently leads to new insights on both sides. Here we describe how knowledge of string theory and M-theory leads to new discoveries about Quantum Information Theory (QIT) and vice-versa (Duff 2007; Kallosh and Linde 2006; Levay 2006). Bekenstein-Hawking entropy Every object, such as a star, has a critical size determined by its mass, which is called the Schwarzschild radius. A black hole is any object smaller than this. Once something falls inside the Schwarzschild radius, it can never escape. This boundary in spacetime is called the event horizon. So the classical picture of a black hole is that of a compact object whose gravitational field is so strong that nothing, not even light, can escape. Yet in 1974 Stephen Hawking showed that quantum black holes are not entirely black but may radiate energy, due to quantum mechanical effects in curved spacetime. In that case, they must possess the thermodynamic quantity called entropy.
    [Show full text]
  • Introduction to Black Hole Entropy and Supersymmetry
    Introduction to black hole entropy and supersymmetry Bernard de Wit∗ Yukawa Institute for Theoretical Physics, Kyoto University, Japan Institute for Theoretical Physics & Spinoza Institute, Utrecht University, The Netherlands Abstract In these lectures we introduce some of the principles and techniques that are relevant for the determination of the entropy of extremal black holes by either string theory or supergravity. We consider such black holes with N =2andN =4 supersymmetry, explaining how agreement is obtained for both the terms that are leading and those that are subleading in the limit of large charges. We discuss the relevance of these results in the context of the more recent developments. 1. Introduction The aim of these lectures is to present a pedagogical introduction to re- cent developments in string theory and supergravity with regard to black hole entropy. In the last decade there have been many advances which have thoroughly changed our thinking about black hole entropy. Supersymmetry has been an indispensable ingredient in all of this, not just because it is an integral part of the theories we consider, but also because it serves as a tool to keep the calculations tractable. Comparisons between the macroscopic and the microscopic entropy, where the latter is defined as the logarithm of the degeneracy of microstates of a certain brane or string configuration, were first carried out in the limit of large charges, assuming the Bekenstein- Hawking area law on the macroscopic (supergravity) side. Later on also subleading corrections could be evaluated on both sides and were shown to be in agreement, although the area law ceases to hold.
    [Show full text]
  • Spin Rate of Black Holes Pinned Down
    IN FOCUS NEWS 449–451; 2013) that used data from NASA’s NuSTAR mission, which was launched last year (see Nature 483, 255; 2012). Study leader Guido Risaliti, an astronomer at the Harvard-Smith- JPL-CALTECH/NASA sonian Center for Astrophysics in Cambridge, Massachusetts, says that NuSTAR provides access to higher-energy X-rays, which has allowed researchers to clarify the influence of the black hole’s gravity on the iron line. These rays are less susceptible than lower-energy X-rays to absorption by clouds of gas between the black hole and Earth, which some had speculated was the real cause of the distortion. In the latest study, astronomers calculated spin more directly (C. Done et al. Mon. Not. R. Astron. Soc. http://doi.org/nc2; 2013). They found a black hole some 150 million parsecs away with a mass 10 million times that of the Sun. Using the European Space Agency’s X-rays emitted by swirling disks of matter hint at the speed at which a supermassive black hole spins. XMM-Newton satellite, they focused not on the iron line but on fainter, lower-energy ASTROPHYSICS X-rays emitted directly from the accretion disk. The spectral shape of these X-rays offers indirect information about the temperature of the innermost part of the disk — and the Spin rate of black temperature of this material is, in turn, related to the distance from the event horizon and the speed at which the black hole is spinning. The calculations suggest that, at most, the black holes pinned down hole is spinning at 86% of the speed of light.
    [Show full text]
  • Kaluza-Klein Theory, Ads/CFT Correspondence and Black Hole Entropy
    View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server IFIC–01–37 Kaluza-Klein theory, AdS/CFT correspondence and black hole entropy J.M. Izquierdoa1, J. Navarro-Salasb1 and P. Navarrob 1 a Departamento de F´ısica Te´orica, Universidad de Valladolid E{47011 Valladolid, Spain b Departamento de F´ısica Te´orica, Universidad de Valencia and IFIC, Centro Mixto Universidad de Valencia{CSIC E{46100 Burjassot (Valencia), Spain Abstract The asymptotic symmetries of the near-horizon geometry of a lifted (near-extremal) Reissner-Nordstrom black hole, obtained by inverting the Kaluza-Klein reduction, explain the deviation of the Bekenstein- Hawking entropy from extremality. We point out the fact that the extra dimension allows us to justify the use of a Virasoro mode decom- position along the time-like boundary of the near-horizon geometry, AdS Sn, of the lower-dimensional (Reissner-Nordstrom) spacetime. 2× 1e-mails: [email protected], [email protected]fic.uv.es, [email protected]fic.uv.es 1 1 Introduction The universality of the Bekenstein-Hawking area law of black holes could be explained if the density of the microscopic states is controlled by the con- formal symmetry [1]. A nice example of this philosophy is provided by the BTZ black holes [2]. The Bekenstein-Hawking entropy can be derived [3], via Cardy’s formula, from the two-dimensional conformal symmetry arising at spatial infinity of three-dimensional gravity with a negative cosmological constant [4]. Moreover, one can look directly at the black hole horizon and treat it as a boundary.
    [Show full text]
  • 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.
    [Show full text]
  • Thermodynamics of Stationary Axisymmetric Einstein-Maxwell Dilaton-Axion Black Hole Jiliang Jing CCAST (Worm Laboratory), P.O
    http://www.paper.edu.cn NUCLEAR PHYSICS B ELSEVIER Nuclear Physics B 476 (1996) 548-555 Thermodynamics of stationary axisymmetric Einstein-Maxwell dilaton-axion black hole Jiliang Jing CCAST (Worm Laboratory), P.O. Box 8730, Beijing 100080, China and Institute of Physics and Physics Department l, Hunan Normal University, Changsha, Hunan 410081, China Received 21 March 1996; accepted 23 April 1996 Abstract The thermodynamics of a stationary axisymmetric Einstein-Maxwell dilaton-axion (EMDA) black hole is investigated using general statistical physics methods. It is shown that entropy and energy have the same form as for the Kerr-Newman charged black hole, but temperature, heat capacity and chemical potential have a different form. However, it is shown that the Bardeen- Carter-Hawking laws of black hole thermodynamics are valid for the stationary axisymmetric EMDA black hole. The black hole possesses second-order phase transitions as does the Kerr- Newman black hole because its heat capacity diverges but both the Helmholtz free energy and entropy are continuous at some value of J and Q. Another interesting result is that the action I can be expressed as I=S+ ~rh J for general stationary black holes in which the external material contribution to mass and angular momentum vanishes. When J = 0, i.e., for static black holes, the result reduces to I = S. PACS: 04.60.+n; 97.60.Lf; 04.65.+e; ll.17.+y 1. Introduction Recently a lot of interest has arosen in obtaining classical dilaton-axion black hole solutions in string theory and investigating their properties [1-4]. In particular attention was focused on the thermodynamics of these black holes.
    [Show full text]
  • Four-Dimensional Black Holes with Scalar Hair in Nonlinear Electrodynamics
    Eur. Phys. J. C (2016) 76:677 DOI 10.1140/epjc/s10052-016-4526-6 Regular Article - Theoretical Physics Four-dimensional black holes with scalar hair in nonlinear electrodynamics José Barrientos1,2,a, P. A. González3,b, Yerko Vásquez4,c 1 Departamento de Física, Universidad de Concepción, Casilla 160-C, Concepción, Chile 2 Departamento de Enseñanza de las Ciencias Básicas, Universidad Católica del Norte, Larrondo 1281, Coquimbo, Chile 3 Facultad de Ingeniería, Universidad Diego Portales, Avenida Ejército Libertador 441, Casilla 298-V, Santiago, Chile 4 Departamento de Física y Astronomía, Facultad de Ciencias, Universidad de La Serena, Avenida Cisternas 1200, La Serena, Chile Received: 14 June 2016 / Accepted: 21 November 2016 © The Author(s) 2016. This article is published with open access at Springerlink.com Abstract We consider a gravitating system consisting of 1 Introduction a scalar field minimally coupled to gravity with a self- interacting potential and a U(1) nonlinear electromagnetic Hairy black holes are interesting solutions to Einstein’s the- field. Solving analytically and numerically the coupled sys- ory of gravity and also to certain types of modified gravity tem for both power-law and Born–Infeld type electrodynam- theories. The first attempts to couple a scalar field to gravity ics, we find charged hairy black hole solutions. Then we was done in an asymptotically flat spacetime finding hairy study the thermodynamics of these solutions and we find black hole solutions [1–3], but it was realized that these solu- that at a low temperature the topological charged black hole tions were not physically acceptable as the scalar field was with scalar hair is thermodynamically preferred, whereas the divergent on the horizon and stability analysis showed that topological charged black hole without scalar hair is thermo- they were unstable [4].
    [Show full text]
  • Black Hole Math Is Designed to Be Used As a Supplement for Teaching Mathematical Topics
    National Aeronautics and Space Administration andSpace Aeronautics National ole M a th B lack H i This collection of activities, updated in February, 2019, is based on a weekly series of space science problems distributed to thousands of teachers during the 2004-2013 school years. They were intended as supplementary problems for students looking for additional challenges in the math and physical science curriculum in grades 10 through 12. The problems are designed to be ‘one-pagers’ consisting of a Student Page, and Teacher’s Answer Key. This compact form was deemed very popular by participating teachers. The topic for this collection is Black Holes, which is a very popular, and mysterious subject among students hearing about astronomy. Students have endless questions about these exciting and exotic objects as many of you may realize! Amazingly enough, many aspects of black holes can be understood by using simple algebra and pre-algebra mathematical skills. This booklet fills the gap by presenting black hole concepts in their simplest mathematical form. General Approach: The activities are organized according to progressive difficulty in mathematics. Students need to be familiar with scientific notation, and it is assumed that they can perform simple algebraic computations involving exponentiation, square-roots, and have some facility with calculators. The assumed level is that of Grade 10-12 Algebra II, although some problems can be worked by Algebra I students. Some of the issues of energy, force, space and time may be appropriate for students taking high school Physics. For more weekly classroom activities about astronomy and space visit the NASA website, http://spacemath.gsfc.nasa.gov Add your email address to our mailing list by contacting Dr.
    [Show full text]
  • Black Hole Entropy Entanglement And
    BLACK HOLE ENTROPY ! ENTANGLEMENT! AND! HOLOGRAPHIC SPACETIME" Ted Jacobson" University of Maryland" Goddard Scientific Colloquium, Feb. 7, 2018 Holographic " Information" principle" paradox" Area 3 4~GN /c geometry" black hole " Einstein eqn " from" entropy" as vacuum " entanglement " thermodynamics" QFT " renormalization" Albert Einstein, aged 33, 1912" GRAVITY IS CURVATURE OF SPACETIME" Spatial curvature analogy:" " Spacetime" Initially parallel lines " don’t stay parallel" time" earth" apple" Time runs slower lower down!" B" Apple free-fall " apple" is the straightest path " in spacetime between A & B…" and the path of longest time." How much slower? " One billionth of a second per year per foot" A" ’ 2 earth" at the earth s surface (g/c )." Spiral of Mercury’s orbit: didn’t fit Newton’s theory, " by 43’’/century…" That’s about 9 minutes advance time for the transit per century… " General relativity nailed it." To calculate the rate of perihelion advance Einstein needed only the first approximation to the line element outside the sun: " " 2 2 2 2 2 2 2 ds = (1− rS r)dt − (1+ rS r)dr − r (dθ +sin θ dϕ ) 2 rS = 2GM c = 3km The Schwarzschild Singularity (1916) 2 2 −1 2 2 2 2 2 ds = (1− rS r)dt − (1− rS r) dr − r (dθ +sin θ dϕ ) 2 rS = 2GM c = 3km "Schwarzschild radius" Schwarzschild (1916): “in order that this discontinuity coincides with the origin” one should define the radial coordinate appropriately. Droste (1916): “a moving particle can never pass that sphere because it would take an infinite amount of time” The true, non-singular nature of the Schwarzschild “singularity” was not widely understood until 42 years later… but it was understood perfectly well by one man in 1932… Georges Lemaitre First person to understand the nature of the Schwarzschild singularity as an event horizon (1932).
    [Show full text]