Determining the Origin and Possible Mechanisms of QPOS in X-Ray Emissions of Neutron Stars and Black Holes Brent Thomson
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Supernovae Sparked by Dark Matter in White Dwarfs
Supernovae Sparked By Dark Matter in White Dwarfs Javier F. Acevedog and Joseph Bramanteg;y gThe Arthur B. McDonald Canadian Astroparticle Physics Research Institute, Department of Physics, Engineering Physics, and Astronomy, Queen's University, Kingston, Ontario, K7L 2S8, Canada yPerimeter Institute for Theoretical Physics, Waterloo, Ontario, N2L 2Y5, Canada November 27, 2019 Abstract It was recently demonstrated that asymmetric dark matter can ignite supernovae by collecting and collapsing inside lone sub-Chandrasekhar mass white dwarfs, and that this may be the cause of Type Ia supernovae. A ball of asymmetric dark matter accumulated inside a white dwarf and collapsing under its own weight, sheds enough gravitational potential energy through scattering with nuclei, to spark the fusion reactions that precede a Type Ia supernova explosion. In this article we elaborate on this mechanism and use it to place new bounds on interactions between nucleons 6 16 and asymmetric dark matter for masses mX = 10 − 10 GeV. Interestingly, we find that for dark matter more massive than 1011 GeV, Type Ia supernova ignition can proceed through the Hawking evaporation of a small black hole formed by the collapsed dark matter. We also identify how a cold white dwarf's Coulomb crystal structure substantially suppresses dark matter-nuclear scattering at low momentum transfers, which is crucial for calculating the time it takes dark matter to form a black hole. Higgs and vector portal dark matter models that ignite Type Ia supernovae are explored. arXiv:1904.11993v3 [hep-ph] 26 Nov 2019 Contents 1 Introduction 2 2 Dark matter capture, thermalization and collapse in white dwarfs 4 2.1 Dark matter capture . -
Arxiv:2101.12220V2 [Astro-Ph.HE]
Neutron Stars Harboring a Primordial Black Hole: Maximum Survival Time Thomas W. Baumgarte1 and Stuart L. Shapiro2, 3 1Department of Physics and Astronomy, Bowdoin College, Brunswick, Maine 04011 2Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801 3Department of Astronomy and NCSA, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801 We explore in general relativity the survival time of neutron stars that host an endoparasitic, possibly primordial, black hole at their center. Corresponding to the minimum steady-state Bondi accretion rate for adiabatic flow that we found earlier for stiff nuclear equations of state (EOSs), we derive analytically the maximum survival time after which the entire star will be consumed by the black hole. We also show that this maximum survival time depends only weakly on the stiffness for polytropic EOSs with Γ ≥ 5/3, so that this survival time assumes a nearly universal value that depends on the initial black hole mass alone. Establishing such a value is important for constraining −16 −10 the contribution of primordial black holes in the mass range 10 M⊙ . M . 10 M⊙ to the dark-matter content of the Universe. Primordial black holes (PBHs) that may have formed the spherical, steady-state, Bondi accretion formula, in the early Universe (see, e.g., [1, 2]) have long been con- M 2ρ sidered candidates for contributing to, if not accounting M˙ =4πλ 0 (1) for, the mysterious and elusive dark matter (see, e.g., [3], a3 as well as [4] for a recent review). Constraints on the PBH contribution to the dark matter have been estab- for adiabatic flow ([18]; see also [19] for a textbook treat- lished by a number of different observations. -
Lecture Notes in Astrophysical Fluid Dynamics
Lecture Notes in Astrophysical Fluid Dynamics Mattia Sormani November 19, 2017 1 Contents 1 Hydrodynamics6 1.1 Introductory remarks..........................6 1.2 The state of a fluid...........................6 1.3 The continuity equation........................7 1.4 The Euler equation, or F = ma ....................8 1.5 The choice of the equation of state.................. 10 1.6 Manipulating the fluid equations................... 14 1.6.1 Writing the equations in different coordinate systems.... 14 1.6.2 Indecent indices......................... 16 1.6.3 Tables of unit vectors and their derivatives.......... 17 1.7 Conservation of energy......................... 18 1.8 Conservation of momentum...................... 21 1.9 Lagrangian vs Eulerian view...................... 21 1.10 Vorticity................................. 22 1.10.1 The vorticity equation..................... 23 1.10.2 Kelvin circulation theorem................... 24 1.11 Steady flow: the Bernoulli's equation................. 26 1.12 Rotating frames............................. 27 1.13 Viscosity and thermal conduction................... 28 1.14 The Reynolds number......................... 33 1.15 Adding radiative heating and cooling................. 35 1.16 Summary................................ 36 1.17 Problems................................. 37 2 Magnetohydrodynamics 38 2.1 Basic equations............................. 38 2.2 Magnetic tension............................ 44 2.3 Magnetic flux freezing......................... 45 2.4 Magnetic field amplification..................... -
Numerical Hydrodynamics in General Relativity
Numerical hydrodynamics in general relativity Jos´eA. Font Departamento de Astronom´ıay Astrof´ısica Edificio de Investigaci´on “Jeroni Mu˜noz” Universidad de Valencia Dr. Moliner 50 E-46100 Burjassot (Valencia), Spain Abstract The current status of numerical solutions for the equations of ideal general rel- ativistic hydrodynamics is reviewed. With respect to an earlier version of the article the present update provides additional information on numerical schemes and extends the discussion of astrophysical simulations in general relativistic hy- drodynamics. Different formulations of the equations are presented, with special mention of conservative and hyperbolic formulations well-adapted to advanced numerical methods. A large sample of available numerical schemes is discussed, paying particular attention to solution procedures based on schemes exploiting the characteristic structure of the equations through linearized Riemann solvers. A comprehensive summary of astrophysical simulations in strong gravitational fields is presented. These include gravitational collapse, accretion onto black holes and hydrodynamical evolutions of neutron stars. The material contained in these sections highlights the numerical challenges of various representative simulations. It also follows, to some extent, the chronological development of the field, concerning advances on the formulation of the gravitational field and arXiv:gr-qc/0003101v2 12 May 2003 hydrodynamic equations and the numerical methodology designed to solve them. 1 Introduction The description -
Bondi-Hoyle Accretion
A Review of Bondi–Hoyle–Lyttleton Accretion Richard Edgar a aStockholms observatorium, AlbaNova universitetscentrum, SE-106 91, Stockholm, Sweden Abstract If a point mass moves through a uniform gas cloud, at what rate does it accrete ma- terial? This is the question studied by Bondi, Hoyle and Lyttleton. This paper draws together the work performed in this area since the problem was first studied. Time has shown that, despite the simplifications made, Bondi, Hoyle and Lyttleton made quite accurate predictions for the accretion rate. Bondi–Hoyle–Lyttleton accretion has found application in many fields of astronomy, and these are also discussed. Key words: accretion PACS: 95.30.Lz, 97.10.Gz, 98.35.Mp, 98.62.Mw 1 Introduction arXiv:astro-ph/0406166v2 21 Jun 2004 In its purest form, Bondi–Hoyle–Lyttleton accretion concerns the supersonic motion of a point mass through a gas cloud. The cloud is assumed to be free of self-gravity, and to be uniform at infinity. Gravity focuses material behind the point mass, which can then accrete some of the gas. This problem has found applications in many areas of astronomy, and this paper is an attempt to address the lack of a general review of the subject. I start with a short summary of the original work of Bondi, Hoyle and Lyt- tleton, followed by a discussion of the numerical simulations performed. Some issues in Bondi–Hoyle–Lyttleton accretion are discussed, before a brief sum- mary of the fields in which the geometry has proved useful. Email address: [email protected] (Richard Edgar). -
Relativistic Emission Lines from Accreting Black Holes
A&A 413, 861–878 (2004) Astronomy DOI: 10.1051/0004-6361:20031522 & c ESO 2004 Astrophysics Relativistic emission lines from accreting black holes The effect of disk truncation on line profiles A. M¨uller and M. Camenzind Landessternwarte Koenigstuhl, 69117 Heidelberg, Germany Received 30 July 2003 / Accepted 22 September 2003 Abstract. Relativistic emission lines generated by thin accretion disks around rotating black holes are an important diagnostic tool for testing gravity near the horizon. The iron K–line is of special importance for the interpretation of the X–ray emission of Seyfert galaxies, quasars and galactic X–ray binary systems. A generalized kinematic model is presented which includes radial drifts and non–Keplerian rotations for the line emitters. The resulting line profiles are obtained with an object–oriented ray tracer operating in the curved Kerr background metric. The general form of the Doppler factor is presented which includes all kinds of poloidal and toroidal motions near the horizon. The parameters of the model include the spin parameter, the inclination, the truncation and outer radius of the disk, velocity profiles for rotation and radial drift, the emissivity profile and a multi–species line–system. The red wing flux is generally reduced when radial drift is included as compared to the pure Keplerian velocity field. All resulting emission line profiles can be classified as triangular, double–horned, double–peaked, bumpy and shoulder–like. Of particular interest are emission line profiles generated by truncated standard accretion disks (TSD). It is also shown that the emissivity law has a great influence on the profiles. -
Arxiv:Astro-Ph/9601106V2 3 Feb 1997
Line Emission from an Accretion Disk around a Rotating Black Hole: Toward a Measurement of Frame Dragging Benjamin C. Bromley1,2, Kaiyou Chen1,3 and Warner A. Miller1 1Theoretical Astrophysics, MS B288, Los Alamos National Laboratory, Los Alamos, NM 87545 2Theoretical Astrophysics, MS-51, Harvard-Smithsonian Center for Astrophysics 60 Garden Street, Cambridge, MA 02138 3Columbia Astrophysics Laboratory, Columbia University, 538 West 120th Street, New York, NY 10027 ABSTRACT Line emission from an accretion disk and a corotating hot spot about a rotating black hole are considered for possible signatures of the frame-dragging effect. We explicitly compare integrated line profiles from a geometrically thin disk about a Schwarzschild and an extreme Kerr black hole, and show that the line profile differences are small if the inner radius of the disk is near or above the Schwarzschild stable-orbit limit of radius 6GM/c2. However, if the inner disk radius extends below this limit, as is pos- sible in the extreme Kerr spacetime, then differences can become significant, especially if the disk emissivity is stronger near the inner regions. We demonstrate that the first three moments of a line profile define a three-dimensional space in which the presence of material at small radii becomes quantitatively evident in broad classes of disk mod- els. In the context of the simple, thin disk paradigm, this moment-mapping scheme suggests formally that the iron line detected by the Advanced Satellite for Cosmology and Astrophysics mission from MCG-6-30-15 (Tanaka et al. 1995) is 3 times more likely to originate from a disk about a rotating black hole than from a Schwarzschild system. -
Accretion Processes on a Black Hole Sandip K
Contents Abstract ........................................... ............. 4 1: Introduction ..................................... .............. 5 1.1 Some General Issues Related to Black Hole Astrophysics . .................. 7 1.1.1 Formation of Black Holes ......................... ....................... 7 1.1.2 Fueling Active Galactic Nuclei . ........................ 9 1.1.3 Evolution of Galactic Centers .................... ....................... 12 1.1.4 Black Holes in Galactic Halos? .................... ..................... 13 1.1.5 Some Signatures of Black Holes .................... ..................... 14 1.2 Difference between Motions around a Newtonian Star and a BlackHole ... 16 1.3 Basics of Pseudo-Newtonian Geometries . .................... 21 1.4 Remarks About Units and Dimensions . .................. 23 2: Spherical Accretion ............................... ............ 24 2.1 Bondi Accretion on a Newtonian Star .................. ................... 25 2.1.1 Basic Equations ................................ ........................ 25 2.1.2 Phase Space Behaviour of the Bondi Flow . ................. 28 2.2 Bondi Flow on a Black Hole ........................... ................... 30 2.2.1 In Schwarzschild Geometry ....................... ....................... 30 2.2.2 In pseudo-Newtonian Geometry .................... ..................... 31 2.3 Bondi Flow with Simple Radiative Transfer . ................... 32 2.4 Bondi Flow with General Radiative Transfer . ................... 32 2.4.1 Single Temperature Solutions -
Brian David Metzger
Curriculum Vitae, Updated 10/20 Brian David Metzger Columbia University Email: [email protected] Department of Physics Web: http://www.columbia.edu/∼bdm2129 909 Pupin Hall, MC 5217 Phone: (212) 854-9702 New York, NY 10027 Fax: (212) 854-3379 ACADEMIC POSITIONS 07/20− Full Professor of Physics, Columbia University 07/19−07/20 Visiting Scholar, Simons Flatiron Institute 01/17−07/20 Associate Professor of Physics, Columbia University 01/13−01/17 Assistant Professor of Physics, Columbia University 09/12−12/12 Lyman Spitzer Jr. Fellow, Princeton University 09/09−12/12 NASA Einstein Fellow, Princeton University EDUCATION 08/03−05/09 University of California at Berkeley M.A. & Ph.D. in Physics (Thesis Adviser: Prof. Eliot Quataert) Dissertation: \Theoretical Models of Gamma-Ray Burst Central Engines" 08/99−05/03 The University of Iowa B.S. in Physics, Astronomy, & Mathematics (Highest Distinction) SELECT HONORS, FELLOWSHIPS and AWARDS 2020 Blavatnik National Laureate in Natural Sciences & Engineering 2020 Simons Investigator in Mathematics and Theoretical Physics 2019 Simons Fellow in Mathematics and Theoretical Physics 2019 2020 Decadal Survey in Astronomy & Astrophysics, Program Panelist 2019 Salpeter Honorary Lecturer, Cornell 2019 Bruno Rossi Prize, American Astronomical Society 2018,19,20 Blavatnik National Awards for Young Scientists, Finalist 2019 New Horizons Breakthrough Prize in Physics 2018 Charles and Thomas Lauritsen Honorary Lecture, Caltech 2016 Scialog Fellow, Research Science Corporation 2014 Alfred P. Sloan Research Fellowship 2009−12 NASA Einstein Fellowship, Princeton 2009 Dissertation Prize, AAS High Energy Astrophysics Division 2009 NASA Hubble Fellowship 2009 Lyman Spitzer Jr. Fellowship, Princeton 2009 Mary Elizabeth Uhl Prize, UC Berkeley Astronomy 2005−08 NASA Graduate Student Research Fellowship 2003 James A. -
Arxiv:2002.12778V2 [Astro-Ph.CO] 9 May 2021 8
CONSTRAINTS ON PRIMORDIAL BLACK HOLES Bernard Carr,1, 2, ∗ Kazunori Kohri,3, 4, 5, y Yuuiti Sendouda,6, z and Jun'ichi Yokoyama2, 5, 7, 8, x 1School of Physics and Astronomy, Queen Mary University of London, Mile End Road, London E1 4NS, UK 2Research Center for the Early Universe (RESCEU), Graduate School of Science, The University of Tokyo, Tokyo 113-0033, Japan 3KEK Theory Center, IPNS, KEK, Tsukuba, Ibaraki 305-0801, Japan 4The Graduate University for Advanced Studies (SOKENDAI), Tsukuba, Ibaraki 305-0801, Japan 5Kavli Institute for the Physics and Mathematics of the Universe, The University of Tokyo, Kashiwa, Chiba 277-8568, Japan 6Graduate School of Science and Technology, Hirosaki University, Hirosaki, Aomori 036-8561, Japan 7Department of Physics, Graduate School of Science, The University of Tokyo, Tokyo 113-0033, Japan 8Trans-scale Quantum Science Institute, The University of Tokyo, Tokyo 113-0033, Japan (Dated: Tuesday 11th May, 2021, 00:43) We update the constraints on the fraction of the Universe that may have gone into primordial black holes (PBHs) over the mass range 10−5{1050 g. Those smaller than ∼ 1015 g would have evaporated by now due to Hawking radiation, so their abundance at formation is constrained by the effects of evaporated particles on big bang nucleosynthesis, the cosmic microwave background (CMB), the Galactic and extragalactic γ-ray and cosmic ray backgrounds and the possible generation of stable Planck mass relics. PBHs larger than ∼ 1015 g are subject to a variety of constraints associated with gravitational lensing, dynamical effects, influence on large-scale structure, accretion and gravitational waves. -
Accretion Onto Black Holes from Large Scales Regulated by Radiative Feedback
Abstract Title of Dissertation: Accretion onto Black Holes from Large Scales Regulated by Radiative Feedback KwangHo Park, Doctor of Philosophy, 2012 Dissertation directed by: Professor Massimo Ricotti Department of Astronomy This thesis focuses on radiation-regulated gas accretion onto black holes (BHs) from galactic scales emphasizing the role of thermal and radiation pressure in lim- iting gas supply to the BH. Assuming quasi-spherical symmetry, we explore how the gas accretion depends on free parameters such as radiative efficiency, BH mass, ambient gas density/temperature, and the spectral index of the radiation. Our nu- merical simulations show an oscillatory behavior of the accretion rate, and thus the luminosity from the BH. We present a model for the feedback loop and provide analytical relationships for the average/maximum accretion rate and the period of the accretion bursts. The thermal structure inside the Str¨omgrensphere is a key factor for the regulation process, while with increasing ambient gas density and mass of BHs, eventually the accretion rate becomes limited by radiation pressure. The period of the luminosity bursts is proportional to the average size of the ionized hot bubble, but we discover that there are two distinct modes of oscillations with very different duty cycles, and that are governed by different depletion processes of the gas inside the ionized bubble. We also study how angular momentum of the gas affects the accretion process. In the second part of the thesis, we study the growth rate and luminosity of BHs in motion with respect to their surrounding medium. We run a large set of two-dimensional axis-symmetric simulations to explore a large parameter space of initial conditions and formulate an analytical model for the accretion. -
Dynamics of Self-Gravitating Disks
University of Cambridge May, 1994 Dynamics of self-gravitating disks Christophe Pichon Clare College and Institute of Astronomy A dissertation submitted to the University of Cambridge in accordance with the regulations for admission to the degree of Doctor of Philosophy ii Summary A fair fraction of observed galactic disks present a bar corresponding to elongated isophotes beyond the central core. Numerical simulations also suggest that bar instabilities are quite common. Why should some galaxies have bars and others not? This question is addressed here by investigating the stability of a self gravitating disk with respect to instabilities induced by the adiabatic re-alignment of resonant orbits. It is shown that the dynamical equations can be recast in terms of the interaction of resonant flows. Concentrating on the stars belonging to the inner Lindblad resonance, it is argued that this interaction yields an instability of Jeans’ type. The Jeans instability traps stars moving in phase with respect to a growing potential; here the azimuthal instability corresponds to a rotating growing potential that captures the lobe of orbital streams of resonant stars. The precession rate of this growing potential is identified with the pattern speed of the bar. The instability criterion puts constraints on the relative dispersion in angular frequency of the underlying distribution function. The outcome of orbital instability is investigated while constructing distribution functions induced by the adiabatic re-alignment of inner Lindblad orbits. These distribution functions maximise entropy while preserving the underlying axisymmetric component of the galaxy and the constraints of angular momentum, total energy, and detailed circulations conservation.