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A Conceptual Model for the Origin of the Cutoff Parameter in Exotic Compact Objects
S S symmetry Article A Conceptual Model for the Origin of the Cutoff Parameter in Exotic Compact Objects Wilson Alexander Rojas Castillo 1 and Jose Robel Arenas Salazar 2,* 1 Departamento de Física, Universidad Nacional de Colombia, Bogotá UN.11001, Colombia; [email protected] 2 Observatorio Astronómico Nacional, Universidad Nacional de Colombia, Bogotá UN.11001, Colombia * Correspondence: [email protected] Received: 30 October 2020; Accepted: 30 November 2020 ; Published: 14 December 2020 Abstract: A Black Hole (BH) is a spacetime region with a horizon and where geodesics converge to a singularity. At such a point, the gravitational field equations fail. As an alternative to the problem of the singularity arises the existence of Exotic Compact Objects (ECOs) that prevent the problem of the singularity through a transition phase of matter once it has crossed the horizon. ECOs are characterized by a closeness parameter or cutoff, e, which measures the degree of compactness of the object. This parameter is established as the difference between the radius of the ECO’s surface and the gravitational radius. Thus, different values of e correspond to different types of ECOs. If e is very big, the ECO behaves more like a star than a black hole. On the contrary, if e tends to a very small value, the ECO behaves like a black hole. It is considered a conceptual model of the origin of the cutoff for ECOs, when a dust shell contracts gravitationally from an initial position to near the Schwarzschild radius. This allowed us to find that the cutoff makes two types of contributions: a classical one governed by General Relativity and one of a quantum nature, if the ECO is very close to the horizon, when estimating that the maximum entropy is contained within the material that composes the shell. -
‰M‰Mwm Cixþvi Cék² I Dîi
gBs‡iwRƒj eBGqi 1g cÎ AwZwiÚ Ask 275 ‰m‰mwm cixÞvi cÉk² I Dîi 1. Dhaka Board-2015 English (Compulsory) 1st Paper Read the passage. Then answer the questions below. The National Memorial at Savar is a symbol of the nation's respect for the martyrs of the War of Liberation. It is built with concrete, but made of blood. It stands 150 feet tall, but every martyr it stands for stands so much taller. It is an achievement the dimension of which can be measured, but it stands for an achievement, which is immeasurable. It stands upright for the millions of martyrs who laid down their lives so that we may stand upright, in honour and dignity, amongst the nations of the world. Most prominently visible is the 150 feet tower that stands on a base measuring 130 feet wide. There are actually a series of 7 towers that rise by stages to a height of 150 feet. The foundation was laid on the first anniversary of the Victory Day. There is actually a plan to build a huge complex in several phases. The entire complex will cover an area of 126 acres. The plan of this complex includes a mosque, a library and a museum. The relics of the Liberation War will be kept in the museum. They will ever remind our countrymen and all who would come to visit museum of the valiant struggle and supreme sacrifices of a freedom loving people. Here also will be a clear warning to all oppressors that the weapons of freedom need not be very big, and that oppression will always be defeated. -
Thesis Rests with Its Author
University of Bath PHD New vacuum solutions for quadratic metric–affine gravity Pasic, Vedad Award date: 2009 Awarding institution: University of Bath Link to publication Alternative formats If you require this document in an alternative format, please contact: [email protected] General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. • Users may download and print one copy of any publication from the public portal for the purpose of private study or research. • You may not further distribute the material or use it for any profit-making activity or commercial gain • You may freely distribute the URL identifying the publication in the public portal ? Take down policy If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. Download date: 23. Sep. 2021 New Vacuum Solutions for Quadratic Metric–affine Gravity submitted by Vedad Pasiˇ c´ for the degree of Doctor of Philosophy of the University of Bath Department of Mathematical Sciences February 2009 COPYRIGHT Attention is drawn to the fact that copyright of this thesis rests with its author. This copy of the thesis has been supplied on the condition that anyone who consults it is understood to recognise that its copyright rests with its author and that no quotation from the thesis and no information derived from it may be published without the prior written consent of the author. -
Fender12 BHB.Pdf
Stellar-Mass Black Holes and Ultraluminous X-ray Sources Rob Fender and Tomaso Belloni Science 337, 540 (2012); DOI: 10.1126/science.1221790 This copy is for your personal, non-commercial use only. If you wish to distribute this article to others, you can order high-quality copies for your colleagues, clients, or customers by clicking here. Permission to republish or repurpose articles or portions of articles can be obtained by following the guidelines here. The following resources related to this article are available online at www.sciencemag.org (this information is current as of March 28, 2013 ): Updated information and services, including high-resolution figures, can be found in the online on March 28, 2013 version of this article at: http://www.sciencemag.org/content/337/6094/540.full.html Supporting Online Material can be found at: http://www.sciencemag.org/content/suppl/2012/08/01/337.6094.540.DC1.html A list of selected additional articles on the Science Web sites related to this article can be found at: http://www.sciencemag.org/content/337/6094/540.full.html#related This article cites 37 articles, 6 of which can be accessed free: www.sciencemag.org http://www.sciencemag.org/content/337/6094/540.full.html#ref-list-1 This article has been cited by 1 articles hosted by HighWire Press; see: http://www.sciencemag.org/content/337/6094/540.full.html#related-urls This article appears in the following subject collections: Astronomy http://www.sciencemag.org/cgi/collection/astronomy Downloaded from Science (print ISSN 0036-8075; online ISSN 1095-9203) is published weekly, except the last week in December, by the American Association for the Advancement of Science, 1200 New York Avenue NW, Washington, DC 20005. -
Effective Conformal Descriptions of Black Hole Entropy
Entropy 2011, 13, 1355-1379; doi:10.3390/e13071355 OPEN ACCESS entropy ISSN 1099-4300 www.mdpi.com/journal/entropy Article Effective Conformal Descriptions of Black Hole Entropy Steven Carlip Department of Physics, University of California at Davis, Davis, CA 95616, USA; E-Mail: [email protected]. Received: 1 July 2011; in revised form: 12 July 2011 / Accepted: 19 July 2011 / Published: 20 July 2011 Abstract: It is no longer considered surprising that black holes have temperatures and entropies. What remains surprising, though, is the universality of these thermodynamic properties: their exceptionally simple and general form, and the fact that they can be derived from many very different descriptions of the underlying microscopic degrees of freedom. I review the proposal that this universality arises from an approximate conformal symmetry, which permits an effective “conformal dual” description that is largely independent of the microscopic details. Keywords: black holes; Bekenstein–Hawking entropy; conformal dual 1. Introduction Since the seminal work of Bekenstein [1] and Hawking [2], we have understood that black holes behave as thermodynamic systems, with characteristic temperatures and entropies. A central task for quantum gravity is finding a statistical mechanical description of this behavior in terms of microscopic states. One important clue may come from the surprising “universality” of these thermodynamic properties, which manifests itself in two ways: – The Bekenstein–Hawking entropy A S = (1) 4G takes the same simple form for all black holes, independent of the charges, spin, and even the number of spacetime dimensions. If the action differs from that of general relativity, the entropy is modified, but again in a simple and universal way [3]. -
Membrane Horizons: the Black Hole's New Clothes
MEMBRANE HORIZONS: THE BLACK HOLE’S NEW CLOTHES Maulik Kirit Parikh A DISSERTATION PRESENTED TO THE FACULTY OF PRINCETON UNIVERSITY IN CANDIDACY FOR THE DEGREE arXiv:hep-th/9907002v1 1 Jul 1999 OF DOCTOR OF PHILOSOPHY RECOMMENDED FOR ACCEPTANCE BY THE DEPARTMENT OF PHYSICS October 1998 Abstract This thesis addresses some classical and semi-classical aspects of black holes, using an effective membrane representation of the event horizon. This “membrane paradigm” is the remarkable view that, to an external observer, a black hole appears to behave exactly like a dynamical fluid membrane, obeying such pre-relativistic equations as Ohm’s law and the Navier-Stokes equation. It has traditionally been derived by manipulating the equations of motion. Here, however, the equations are derived from an underlying action formulation which has the advantage of clarifying the paradigm and simplifying the derivations, in addition to providing a bridge to thermodynamics and quantum mechanics. Within this framework, previous mem- brane results are derived and extended to dyonic black hole solutions. It is explained how an action can produce dissipative equations. The classical portion of the study ends with a demonstration of the validity of a minimum entropy production principle for black holes. Turning next to semi-classical theory, it is shown that familiar thermodynamic properties of black holes also emerge from the membrane action, via a Euclidean path integral. In particular, the membrane action can account for the hole’s Bekenstein- Hawking entropy, including the numerical factor. Two short and direct derivations of Hawking radiation as an instanton process are then presented. The first is a tunneling calculation based on particles in a dynamical geometry, closely analogous to Schwinger pair production in an electric field. -
Energy Extraction from Boosted Black Holes: Penrose Process, Jets, and the Membrane at Infinity
Energy extraction from boosted black holes: Penrose process, jets, and the membrane at infinity The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Penna, Robert F. "Energy extraction from boosted black holes: Penrose process, jets, and the membrane at infinity." Phys. Rev. D 91, 084044 (April 2015). © 2015 American Physical Society As Published http://dx.doi.org/10.1103/PhysRevD.91.084044 Publisher American Physical Society Version Final published version Citable link http://hdl.handle.net/1721.1/96722 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. PHYSICAL REVIEW D 91, 084044 (2015) Energy extraction from boosted black holes: Penrose process, jets, and the membrane at infinity Robert F. Penna* Department of Physics and Kavli Institute for Astrophysics and Space Research, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA (Received 12 March 2015; published 20 April 2015) Numerical simulations indicate that black holes carrying linear momentum and/or orbital momentum can power jets. The jets extract the kinetic energy stored in the black hole’s motion. This could provide an important electromagnetic counterpart to gravitational wave searches. We develop the theory underlying these jets. In particular, we derive the analogues of the Penrose process and the Blandford-Znajek jet power prediction for boosted black holes. The jet power we find is ðv=2MÞ2Φ2=ð4πÞ, where v is the hole’s velocity, M is its mass, and Φ is the magnetic flux. -
Black Holes and Black Hole Thermodynamics Without Event Horizons
General Relativity and Gravitation (2011) DOI 10.1007/s10714-008-0739-9 RESEARCHARTICLE Alex B. Nielsen Black holes and black hole thermodynamics without event horizons Received: 18 June 2008 / Accepted: 22 November 2008 c Springer Science+Business Media, LLC 2009 Abstract We investigate whether black holes can be defined without using event horizons. In particular we focus on the thermodynamic properties of event hori- zons and the alternative, locally defined horizons. We discuss the assumptions and limitations of the proofs of the zeroth, first and second laws of black hole mechan- ics for both event horizons and trapping horizons. This leads to the possibility that black holes may be more usefully defined in terms of trapping horizons. We also review how Hawking radiation may be seen to arise from trapping horizons and discuss which horizon area should be associated with the gravitational entropy. Keywords Black holes, Black hole thermodynamics, Hawking radiation, Trapping horizons Contents 1 Introduction . 2 2 Event horizons . 4 3 Local horizons . 8 4 Thermodynamics of black holes . 14 5 Area increase law . 17 6 Gravitational entropy . 19 7 The zeroth law . 22 8 The first law . 25 9 Hawking radiation for trapping horizons . 34 10 Fluid flow analogies . 36 11 Uniqueness . 37 12 Conclusion . 39 A. B. Nielsen Center for Theoretical Physics and School of Physics College of Natural Sciences, Seoul National University Seoul 151-742, Korea [email protected] 2 A. B. Nielsen 1 Introduction Black holes play a central role in physics. In astrophysics, they represent the end point of stellar collapse for sufficiently large stars. -
On the Nature of the Blandford-Znajek Mechanism
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server ON THE NATURE OF THE BLANDFORD-ZNAJEK MECHANISM Komissarov S.S. Department of Applied Mathematics, University of Leeds, Leeds LS2 9JT, UK. E-mail: [email protected] It is widely accepted in the astrophysical community that the event horizon plays crucial role in the Blandford-Znajek mechanism of extraction of rotational energy of black holes. In fact, this view is a quintessence of the Membrane Paradigm of black holes which suggests that the event horizon, or rather the so-called stretched horizon, is similar to a rotating conducting sphere of finite resistivity. In this paper we argue that this interpretation is rather misleading and the proper explanation of the Blandford-Znajek mechanism has to be sought in the properties of the ergospheric region of black holes. 1 Blandford-Znajek solution and the Membrane Paradigm We start with describing some basic properties of steady-state force-free mag- netospheres of black-holes as discovered in [1] using the 3+1 formulation of electrodynamics. First we introduce vectors of electric and magnetic field as follows 1 E = F Bi = eijkF , (1) i it 2 jk where Fµν is the electromagnetic field tensor,and e is the Levi-Civita alternat- ing tensor. For steady-state axisymmetric solutions Eφ =0.Considerapolar flux tube of magnetic flux i j k Φ= B dSi (dSi = eijkdx dx ) Z (1) (2) The angular velocity of magnetic field lines defined as Ω=E /√γBθ = E /√γBr. -
Introduction to Black Hole Astrophysics, 2010 Gustavo E
Lecture Notes Introduction to Black Hole Astrophysics, 2010 Gustavo E. Romero Introduction to black hole astrophysics Gustavo E. Romero Instituto Argentino de Radioastronomía, C.C. 5, Villa Elisa (1894), and Facultad de Cs. Astronómicas y Geofísicas, UNLP, Paseo del Bosque S/N, (1900) La Plata, Argentina, [email protected] Es cosa averiguada que no se sabe nada, y que todos son ignorantes; y aun esto no se sabe de cierto, que, a saberse, ya se supiera algo: sospéchase. Quevedo Abstract. Black holes are perhaps the most strange and fascinating objects in the universe. Our understanding of space and time is pushed to its limits by the extreme conditions found in these objects. They can be used as natural laboratories to test the behavior of matter in very strong gravitational fields. Black holes seem to play a key role in the universe, powering a wide variety of phenomena, from X-ray binaries to active galactic nuclei. In these lecture notes the basics of black hole physics and astrophysics are reviewed. 1. Introduction Strictly speaking, black holes do not exist. Moreover, holes, of any kind, do not exist. You can talk about holes of course. For instance you can say: “there is a hole in the wall”. You can give many details of the hole: it is big, it is round shaped, light comes in through it. Even, perhaps, the hole could be such that you can go through to the outside. But I am sure that you do not think that there is a thing made out of nothingness in the wall. -
Membrane Paradigm, Gravitational Θ-Term and Gauge/Gravity Duality
UTTG-21-15 TCC-010-15 Membrane Paradigm, Gravitational Θ-Term and Gauge/Gravity Duality Willy Fischlera;b, Sandipan Kunduc aTheory Group, Department of Physics, University of Texas, Austin, TX 78712, USA bTexas Cosmology Center, University of Texas, Austin, TX 78712, USA cDepartment of Physics, Cornell University, Ithaca, New York, 14853, USA E-mail: [email protected], [email protected] Abstract: Following the membrane paradigm, we explore the effect of the gravitational Θ-term on the behavior of the stretched horizon of a black hole in (3 + 1)-dimensions. We reformulate the membrane paradigm from a quantum path-integral point of view where we interpret the macroscopic properties of the horizon as effects of integrating out the region inside the horizon. The gravitational Θ-term is a total derivative, how- ever, using our framework we show that this term affects the transport properties of the horizon. In particular, the horizon acquires a third order parity violating, dimensionless transport coefficient which affects the way localized perturbations scramble on the hori- zon. Then we consider a large-N gauge theory in (2 + 1)−dimensions which is dual to an asymptotically AdS background in (3 + 1)−dimensional spacetime to show that the Θ-term induces a non-trivial contact term in the energy-momentum tensor of the dual theory. As a consequence, the dual gauge theory in the presence of the Θ-term acquires the same third order parity violating transport coefficient. arXiv:1512.01238v2 [hep-th] 13 May 2016 Contents 1 Introduction1 2 Integrating -
Atomic-Scientists.Pdf
Table of Contents Becquerel, Henri Blumgart, Herman Bohr, Niels Chadwick, James Compton, Arthur Coolidge, William Curie, Marie Curie, Pierre Dalton, John de Hevesy, George Einstein, Albert Evans, Robely Failla, Gioacchino Fermi, Enrico Frisch, Otto Geiger, Hans Goeppert-Mayer, Maria Hahn, Otto Heisenberg, Werner Hess, Victor Francis Joliet-Curie, Frederic Joliet-Curie, Irene Klaproth, Martin Langevin, Paul Lawrence, Ernest Meitner, Lise Millikan, Robert Moseley, Henry Muller, Hermann Noddack, Ida Parker, Herbert Peierls, Rudolf Quimby, Edith Ray, Dixie Lee Roentgen, Wilhelm Rutherford, Ernest Seaborg, Glenn Soddy, Frederick Strassman, Fritz Szilard, Leo Teller, Edward Thomson, Joseph Villard, Paul Yalow, Rosalyn Antoine Henri Becquerel 1852 - 1908 French physicist who was an expert on fluorescence. He discovered the rays emitted from the uranium salts in pitchblende, called Becquerel rays, which led to the isolation of radium and to the beginning of modern nuclear physics. He shared the 1903 Nobel Prize for Physics with Pierre and Marie Curie for the discovery of radioactivity.1 Early Life Antoine Henri Becquerel was born in Paris, France on December 15, 1852.3 He was born into a family of scientists and scholars. His grandfather, Antoine Cesar Bequerel, invented an electrolytic method for extracting metals from their ores. His father, Alexander Edmond Becquerel, a Professor of Applied Physics, was known for his research on solar radiation and on phosphorescence.2, 3 Becquerel not only inherited their interest in science, but he also inherited the minerals and compounds studied by his father, which gave him a ready source of fluorescent materials in which to pursue his own investigations into the mysterious ways of Wilhelm Roentgen’s newly discovered phenomenon, X-rays.2 Henri received his formal, scientific education at Ecole Polytechnique in 1872 and attended the Ecole des Ponts at Chaussees from 1874-77 for his engineering training.