Binary Black Holes Tell Us How Fast the Universe Is Expanding
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Life and Adventures of Binary Supermassive Black Holes
Life and adventures of binary supermassive black holes Eugene Vasiliev Lebedev Physical Institute Plan of the talk • Why binary black holes? • Evolutionary stages: – galaxy merger and dynamical friction: the first contact – king of the hill: the binary hardens – the lean years: the final parsec problem – runaway speedup: gravitational waves kick in – anschluss • Life after merger • Perspectives of detection Origin of binary supermassive black holes • Most galaxies are believed to host central massive black holes • In the hierarchical merger paradigm, galaxies in the Universe have typically 1-3 major and multiple minor mergers in their lifetime • Every such merger brings two central black holes from parent galaxies together to form a binary system • We don’t see much evidence for widespread binary SMBH (to say the least) – therefore they need to merge rather efficiently • Merger is a natural way of producing huge black holes from smaller seeds Evolutionary track of binary SMBH • Merger of two galaxies creates a common nucleus; dynamical friction rapidly brings two black holes together to form a binary (a~10 pc) • Three-body interaction of binary with stars of galactic nucleus ejects most stars from the vicinity of the binary by the slingshot effect; a “mass deficit” is created and the binary becomes “hard” (a~1 pc) • The binary further shrinks by scattering off stars that continue to flow into the “loss cone”, due to two-body relaxation or other factors • As the separation reaches ~10–2 pc, gravitational wave emission becomes the dominant mechanism that carries away the energy • Reaching a few Schwarzschild radii (~10–5 pc), the binary finally merges Evolution timescales I. -
Binary Black Holes: an Introduction
Binary Black Holes: An Introduction Roger Blandford KIPAC Stanford 29 xi 2012 Tucson 1 Inertial Confinement of Extended Radio Sources Three‐Dimensional Magnetohydrodynamic Simulations of Buoyant Bubbles in Galaxy Clusters De Young and Axford 1967, Nature O’Neill, De Young and Jones 2011 29 xi 2012 Tucson 2 Mergers and Acquisitions • Mpc Problem • kpc Problem • pc Problem • mpc Problem 29 xi 2012 Tucson 3 The Megaparsec Problem • Galaxies with Spheroids have massive black holes (MBH) 4 -3 – m8~σ200 ; m ~ 10 Msph – Evolution? (Treu et al) • Galaxies assembled through hierarchical mergers of DM halos. – Major and minor – Halo Occupation Density Mayer – DM simulations quantitative; gas messy 29 xi 2012 Tucson 4 Can we calculate R(m1,m2,z,ρ…)? Energy self-sufficiency? • Kocevski eg (2012) [CANDELS] – Modest power – X-ray selected – Imaged in NIR – z~2 • AGN – ~0.5 in disks; ~0.3 in spheroids – >0.8 undisturbed like control sample • Selection effects rampant! – Opposite conclusions drawn from other studies 29 xi 2012 Tucson 5 How do we ask the right questions observationally? The kiloparsec Problem • Circum-Nuclear Disks – ULIRGs ~ 100pc – Sgr A* ~ 1 pc • Invoked to supply friction – Is it necessary for merger? 29 xi 2012 Tucson 6 Max et al Double AGN • Sample – SDSSIII etc – Double-peaked spectra • O[III] 5007 ΔV ~ 300-1000 km s-1 Blecha – Adaptive optics – X-rays, radio – Spectra • Are they outflows/jets/NLR? Double gas, disks, holes, NLR? 29 xi 2012 Tucson 7 Deadbeat Dads? • Are quasars mergers of two gas-rich galaxies • Is there a deficit -
Stochastic Gravitational Wave Backgrounds
Stochastic Gravitational Wave Backgrounds Nelson Christensen1;2 z 1ARTEMIS, Universit´eC^oted'Azur, Observatoire C^oted'Azur, CNRS, 06304 Nice, France 2Physics and Astronomy, Carleton College, Northfield, MN 55057, USA Abstract. A stochastic background of gravitational waves can be created by the superposition of a large number of independent sources. The physical processes occurring at the earliest moments of the universe certainly created a stochastic background that exists, at some level, today. This is analogous to the cosmic microwave background, which is an electromagnetic record of the early universe. The recent observations of gravitational waves by the Advanced LIGO and Advanced Virgo detectors imply that there is also a stochastic background that has been created by binary black hole and binary neutron star mergers over the history of the universe. Whether the stochastic background is observed directly, or upper limits placed on it in specific frequency bands, important astrophysical and cosmological statements about it can be made. This review will summarize the current state of research of the stochastic background, from the sources of these gravitational waves, to the current methods used to observe them. Keywords: stochastic gravitational wave background, cosmology, gravitational waves 1. Introduction Gravitational waves are a prediction of Albert Einstein from 1916 [1,2], a consequence of general relativity [3]. Just as an accelerated electric charge will create electromagnetic waves (light), accelerating mass will create gravitational waves. And almost exactly arXiv:1811.08797v1 [gr-qc] 21 Nov 2018 a century after their prediction, gravitational waves were directly observed [4] for the first time by Advanced LIGO [5, 6]. -
Supermassive Black-Hole Demographics & Environments
Astro2020 Science White Paper Supermassive Black-hole Demographics & Environments With Pulsar Timing Arrays Principal authors Stephen R. Taylor (California Institute of Technology), [email protected] Sarah Burke-Spolaor (West Virginia University/Center for Gravitational Waves and Cosmology/CIFAR Azrieli Global Scholar), [email protected] Co-authors • Paul T. Baker (West Virginia University) • Maria Charisi (California Institute of Technology) • Kristina Islo (University of Wisconsin-Milwaukee) • Luke Z. Kelley (Northwestern University) • Dustin R. Madison (West Virginia University) • Joseph Simon (Jet Propulsion Laboratory, California Institute of Technology) • Sarah Vigeland (University of Wisconsin-Milwaukee) This is one of five core white papers written by members of the NANOGrav Collaboration. Related white papers • Nanohertz Gravitational Waves, Extreme Astrophysics, And Fundamental Physics With arXiv:1903.08183v1 [astro-ph.GA] 19 Mar 2019 Pulsar Timing Arrays, J. Cordes, M. McLaughlin, et al. • Fundamental Physics With Radio Millisecond Pulsars, E. Fonseca, et al. • Physics Beyond The Standard Model With Pulsar Timing Arrays, X. Siemens, et al. • Multi-messenger Astrophysics With Pulsar-timing Arrays, L. Z. Kelley, et al. Thematic Areas: Planetary Systems Star and Planet Formation Formation and Evolution of Compact Objects X Cosmology and Fundamental Physics Stars and Stellar Evolution Resolved Stellar Populations and their Environments X Galaxy Evolution X Multi-Messenger Astronomy and Astrophysics 1 Science Opportunity: Probing the Supermassive Black Hole Population With Gravitational Waves 6 9 With masses in the range 10 {10 M , supermassive black holes (SMBHs) are the most massive compact objects in the Universe. They lurk in massive galaxy centers, accreting inflowing gas, and powering jets that regulate their further accretion as well as galactic star formation. -
Gravitational Waves from Binary Supermassive Black Holes Missing in Pulsar Observations Authors: R
Gravitational waves from binary supermassive black holes missing in pulsar observations Authors: R. M. Shannon1,2*, V. Ravi3*, L. T. Lentati4, P. D. Lasky5, G. Hobbs1, M. Kerr1, R. N. Manchester1, W. A. Coles6, Y. Levin5, M. Bailes3, N. D. R. Bhat2, S. Burke-Spolaor7, S. Dai1,8, M. J. Keith9, S. Osłowski10,11, D. J. Reardon5, W. van Straten3, L. Toomey1, J.-B. Wang12, L. Wen13, J. S. B. Wyithe14, X.-J. Zhu13 Affiliations: 1 CSIRO Astronomy and Space Science, Australia Telescope National Facility, P.O. Box 76, Epping, NSW 1710, Australia. 2 International Centre for Radio Astronomy Research, Curtin University, Bentley, WA 6102, Australia. 3 Centre for Astrophysics and Supercomputing, Swinburne University of Technology, PO Box 218, Hawthorn, VIC 3122, Australia. 4 Astrophysics Group, Cavendish Laboratory, JJ Thomson Avenue, Cambridge CB3 0HE, UK. 5 Monash Centre for Astrophysics, School of Physics and Astronomy, Monash University, PO Box 27, VIC 3800, Australia. 6 Department of Electrical and Computer Engineering, University of California at San Diego, La Jolla, CA 92093, USA. 7 National Radio Astronomical Observatory, Array Operations Center, P.O. Box O, Socorro, NM 87801-0387, USA. 8 Department of Astronomy, School of Physics, Peking University, Beijing, 100871, China. 9 Jodrell Bank Centre for Astrophysics, University of Manchester, M13 9PL, UK. 10 Department of Physics, Universitat Bielefeld, Universitatsstr 25, D-33615 Bielefeld, Germany. 11 Max-Planck-Institut für Radioastronomie, Auf dem Hügel 69, 53121 Bonn, Germany. 12 Xinjiang Astronomical Observatory, CAS, 150 Science 1-Street, Urumqi, Xinjiang 830011, China. 13 School of Physics, University of Western Australia, Crawley, WA 6009, Australia. -
Trumpet Initial Data for Highly Boosted Black Holes and High Energy Binaries
TRUMPET INITIAL DATA FOR HIGHLY BOOSTED BLACK HOLES AND HIGH ENERGY BINARIES Kyle Patrick Slinker A dissertation submitted to the faculty at the University of North Carolina at Chapel Hill in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the Department of Physics and Astronomy. Chapel Hill 2017 Approved by: Charles R. Evans J. Christopher Clemens Louise A. Dolan Joaqu´ınE. Drut Fabian Heitsch Reyco Henning c 2017 Kyle Patrick Slinker ALL RIGHTS RESERVED ii ABSTRACT Kyle Patrick Slinker: Trumpet Initial Data for Highly Boosted Black Holes and High Energy Binaries (Under the direction of Charles R. Evans) Initial data for a single boosted black hole is constructed that analytically contains no initial transient (junk) gravitational radiation and is adapted to the moving punctures gauge conditions. The properties of this data are investigated in detail. It is found to be generally superior to canonical Bowen-York data and, when implemented numerically in simulations, yields orders of magnitude less junk gravitational radiation content and more accurate black hole velocities. This allows for modeling of black holes that are boosted faster than previously possible. An approximate superposition of the data is used to demonstrate how a binary black hole system can be constructed to retain the advantages found for the single black hole. Extensions to black holes with spin are considered. iii TABLE OF CONTENTS LIST OF TABLES ............................................. vii LIST OF FIGURES ............................................ viii LIST OF ABBREVIATIONS AND SYMBOLS ........................... xii 1 Introduction ............................................... 1 1.1 Testing General Relativity Through Gravitational Wave Astronomy . 1 1.2 Numerical Relativity . 2 1.3 Project Goals . -
The Historical 1900 and 1913 Outbursts of the Binary Blazar Candidate OJ287
A&A 559, A20 (2013) Astronomy DOI: 10.1051/0004-6361/201219323 & c ESO 2013 Astrophysics The historical 1900 and 1913 outbursts of the binary blazar candidate OJ287 R. Hudec1,2, M. Bašta3,P.Pihajoki4, and M. Valtonen5 1 Astronomical Institute, Academy of Sciences of the Czech Republic, Fricovaˇ 298, 251 65 Ondrejov,ˇ Czech Republic e-mail: [email protected] 2 Czech Technical University, Faculty of Electrical Engineering, Technicka 2, 160 00 Praha 6, Czech Republic 3 Faculty of Informatics and Statistics, University of Economics, 130 67 Prague, Czech Republic 4 Department of Physics and Astronomy, University of Turku, 21500 Piikkio, Finland 5 Finnish Centre for Astronomy with ESO, University of Turku, 21500 Piikkio, Finland Received 31 March 2012 / Accepted 14 February 2013 ABSTRACT We report on historical optical outbursts in the OJ287 system in 1900 and 1913, detected on archival astronomical plates of the Harvard College Observatory. The 1900 outburst is reported for the first time. The first recorded outburst of the periodically active quasar OJ287 described before was observed in 1913. Up to now the information on this event was based on three points from plate archives. We used the Harvard plate collection, and added another seven observations to the light curve. The light curve is now well covered and allows one to determine the beginning of the outburst quite accurately. The outburst was longer and more energetic than the standard 1983 outburst. Should the system be strictly periodic, the period determined from these two outbursts would be 11.665 yr. However, this does not match the 1900 outburst or other prominent outbursts in the record. -
Pos(AASKA14)151
Multiple supermassive black hole systems: SKA’s future leading role PoS(AASKA14)151 Roger Deane∗1;2, Zsolt Paragi3, Matt Jarvis4;5, Mickäel Coriat1;2, Gianni Bernardi2;6;7, Sandor Frey8, Ian Heywood9;6, Hans-Rainer Klöckner10 1 University of Cape Town, 2 Square Kilometre Array South Africa, 3 Joint Institute for VLBI in Europe, 4 University of Oxford, 5 University of the Western Cape, 6 Rhodes University, 7 Harvard-Smithsonian Center for Astrophysics, 8 FÖMI Satellite Geodetic Observatory, 9 CSIRO Astronomy and Space Science, 10 Max-Planck-Institut für Radioastronomie E-mail: roger.deane [at] ast.uct.ac.za Galaxies and supermassive black holes (SMBHs) are believed to evolve through a process of hierarchical merging and accretion. Through this paradigm, multiple SMBH systems are expected to be relatively common in the Universe. However, to date there are poor observational constraints on multiple SMBHs systems with separations comparable to a SMBH gravitational sphere of influence (« 1 kpc). In this chapter, we discuss how deep continuum observations with the SKA will make leading contributions towards understanding how multiple black hole systems impact galaxy evolution. In addition, these observations will provide constraints on and an understanding of stochastic gravitational wave background detections in the pulsar timing array sensitivity band (nHz -mHz). We also discuss how targets for pointed gravitational wave experiments (that cannot be resolved by VLBI) could potentially be found using the large-scale radio-jet morphology, which can be modulated by the presence of a close-pair binary SMBH system. The combination of direct imaging at high angular resolution; low-surface brightness radio-jet tracers; and pulsar timing arrays will allow the SKA to trace black hole binary evolution from separations of a galaxy virial radius down to the sub-parsec level. -
A RADIO RELIC and a SEARCH for the CENTRAL BLACK HOLE in the ABELL 2261 BRIGHTEST CLUSTER GALAXY Sarah Burke-Spolaor1,2,3,4 Kayhan Gultekin¨ 5, Marc Postman6, Tod R
Faculty Scholarship 2017 A Radio Relic And A Search For The eC ntral Black Hole In The Abell 2261 Brightest Cluster Galaxy Sarah Burke-Spolaor Kayhan Gültekin Marc Postman Tod R. Lauer Joanna M. Taylor See next page for additional authors Follow this and additional works at: https://researchrepository.wvu.edu/faculty_publications Digital Commons Citation Burke-Spolaor, Sarah; Gültekin, Kayhan; Postman, Marc; Lauer, Tod R.; Taylor, Joanna M.; Lazio, T. Joseph W.; and Moustakas, Leonidas A., "A Radio Relic And A Search For The eC ntral Black Hole In The Abell 2261 Brightest Cluster Galaxy" (2017). Faculty Scholarship. 448. https://researchrepository.wvu.edu/faculty_publications/448 This Article is brought to you for free and open access by The Research Repository @ WVU. It has been accepted for inclusion in Faculty Scholarship by an authorized administrator of The Research Repository @ WVU. For more information, please contact [email protected]. Authors Sarah Burke-Spolaor, Kayhan Gültekin, Marc Postman, Tod R. Lauer, Joanna M. Taylor, T. Joseph W. Lazio, and Leonidas A. Moustakas This article is available at The Research Repository @ WVU: https://researchrepository.wvu.edu/faculty_publications/448 Draft version September 5, 2018 Preprint typeset using LATEX style emulateapj v. 12/16/11 A RADIO RELIC AND A SEARCH FOR THE CENTRAL BLACK HOLE IN THE ABELL 2261 BRIGHTEST CLUSTER GALAXY Sarah Burke-Spolaor1,2,3,4 Kayhan Gultekin¨ 5, Marc Postman6, Tod R. Lauer7, Joanna M. Taylor6, T. Joseph W. Lazio8, and Leonidas A. Moustakas8 Draft version September 5, 2018 ABSTRACT We present VLA images and HST/STIS spectra of sources within the center of the brightest cluster galaxy (BCG) in Abell 2261. -
New Physics and the Black Hole Mass Gap
New physics and the Black Hole Mass Gap Djuna Lize Croon (TRIUMF) University of Michigan, September 2020 [email protected] | djunacroon.com GW190521 LIGO/Virgo’s biggest discovery yet: the impossible black holes Phys. Rev. Le?. 125, 101102 (2020). From R. Abbo? et al. (LIGO ScienCfic CollaboraCon and Virgo CollaboraCon), GW190521 LIGO/Virgo’s biggest discovery yet: the impossible black holes Phys. Rev. Le?. 125, 101102 (2020). From R. Abbo? et al. (LIGO ScienCfic CollaboraCon and Virgo CollaboraCon), GW190521 LIGO/Virgo’s biggest discovery yet: the impossible black holes … let’s wind back a bit “The Stellar Binary mergers in LIGO/Virgo O1+O2 Graveyard” Adapted from LIGO-Virgo, Frank Elavsky, Aaron Geller “The Stellar Binary mergers in LIGO/Virgo O1+O2 Graveyard” Mass Gap? “Mass Gap” Adapted from LIGO-Virgo, Frank Elavsky, Aaron Geller What populates the stellar graveyard? • In the LIGO/Virgo mass range: remnants of heavy, low-metallicity population-III stars • Primarily made of hydrogen (H) and helium (He) • Would have existed for z ≳ 6, M ∼ 20 − 130 M⊙ • Have not been directly observed yet (JWST target) • Collapsed into black holes in core-collapse supernova explosions. (Or did they?) • We study their evolution from the Zero-Age Helium Branch (ZAHB) <latexit sha1_base64="PYrKTlHPDF1/X3ZrAR6z/bngQPE=">AAACBHicdVDLSgMxFM34rPU16rKbYBFcDTN1StuFUHTjplDBPqAtQyZN29BMMiQZoQxduPFX3LhQxK0f4c6/MX0IKnrgwuGce7n3njBmVGnX/bBWVtfWNzYzW9ntnd29ffvgsKlEIjFpYMGEbIdIEUY5aWiqGWnHkqAoZKQVji9nfuuWSEUFv9GTmPQiNOR0QDHSRgrsXC1IuzKClE/PvYI757Vp0BV9oQM77zquXywWPeg6Z5WS75cNqZS8sleBnuPOkQdL1AP7vdsXOIkI15ghpTqeG+teiqSmmJFptpsoEiM8RkPSMZSjiKheOn9iCk+M0ocDIU1xDefq94kURUpNotB0RkiP1G9vJv7ldRI9KPdSyuNEE44XiwYJg1rAWSKwTyXBmk0MQVhScyvEIyQR1ia3rAnh61P4P2kWHM93Ktd+vnqxjCMDcuAYnAIPlEAVXIE6aAAM7sADeALP1r31aL1Yr4vWFWs5cwR+wHr7BCb+l9Y=</latexit> -
LIGO Listens for Gravitational Waves
LIGO-Virgo Gravitational-Wave Findings So Far, and Current Events Peter S. Shawhan University of Maryland Physics Department and Joint Space-Science Institute University of Maryland APS Mid-Atlantic Senior Physicists Group February 19, 2020 1 LIGO = Laser Interferometer Gravitational-wave Observatory LIGO Hanford Observatory Two LIGO Observatories LIGO Hanford LIGO Livingston Observatory Plus the Virgo Observatory in Italy Having three detectors significantly improves our ability to confidently detect weak sources and to locate them in the sky 4 Improving detectors over time to reduce the noise level Initial LIGO (2002-2010) Advanced LIGO (as of 2015) 10−23 amplitude spectral density! LIGO-G1501223-v3 5 Advanced Detector Observing Runs O1 — September 12, 2015 to January 19, 2016 LIGO Hanford and Livingston O2 — November 30, 2016 to August 25, 2017 Initially, just the two LIGO observatories Virgo joined on August 1, 2017 O3 — Began April 1, 2019 Both LIGO observatories plus Virgo 6 Ten binary black hole mergers detected in O1+O2! Browse events at https://ligo.northwestern.edu/media/mass-plot/index.html 7 Highlights: Binary Black Hole Mergers Exploring the Properties of GW Events Bayesian parameter estimation: Adjust physical parameters of waveform model to see what fits the data from all detectors well Illustration by N. Cornish and T. Littenberg Get ranges of likely (“credible”) parameter values 9 Population of Merging BBHs: Masses Mass ratio (풒) consistent with 1 for all these events, but with significant uncertainty The data determines “chirp mass” best for low-mass BBHs, and total mass best for high-mass BBHs [Abbott et al. -
Gamma Ray Bursts from Binary Black Holes
Gamma ray bursts from binary black holes Agnieszka Janiuk Center for Theoretical Physics, Polish Academy of Sciences, Warsaw Collaboration: Szymon Charzyński (Warsaw University) Michał Bejger (Copernicus Astronomical Center, Warsaw) www.cft.edu.pl A&A, 2013, 560, 25 Gamma Ray Bursts Prompt emission in Gamma, late-time emission with X-rays Energetic explosions connected with collapse of massive stars or compact object mergers Especially interesting is scenario when two compact objects merge within a collapsar Electromagnetic signal accompanied by gravitational waves We unify the two “standard” models Massive star explosion and mass fallback from the envelope Paczyński (1998); McFadyen & Compact binary merger: neutron Woosley (1999) star disruption Eichler et al. (1989); Ruffert & Janka (1999) Compact companion enters the massive star's envelope Common envelope phase, transient phase (analog of a Thorne-Żytkov object) Trigger of the core collapse, SN (Hypernova) explosion -> GRB Ultimate fate of HMXBs: Binary pulsar NS-BH BH-BH Possible progenitors: known high mass X-ray binaries Close binary: massive OB star plus compact remnant Examples: Cyg X-3, IC 10 X-1, NGC 300 X-1, M33 X-7 Statistics: the advanced LIGO/VIRGO detection rate of BH-BH mergers from Cyg X-3 formation channel is estimated at 10 yr-1 BH HMXBs formed at z>6 might have impact on cosmic reionisation. Their Zhang & Fryer (2001); Barkov & fraction should increase with redshift Komissarov (2010); Church et al. (2012); Belczyński et al. (2013); Mirabel et al (2011) Our scenario