Physics for Everyone: How to Explain Gravitational Waves to a Lay Audience
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GW170104: Observation of a 50-Solar-Mass Binary Black Hole Coalescence at Redshift 0.2 – Supplemental Material
GW170104: Observation of a 50-Solar-Mass Binary Black Hole Coalescence at Redshift 0.2 { Supplemental Material The LIGO Scientific Collaboration and the Virgo Collaboration I. NOISE PERFORMANCE OF THE sis used an initial calibration of the data and assumed DETECTORS a (conservative) one-sigma calibration uncertainty of 10% in amplitude and 10◦ in phase for both detec- Figure 1 shows a comparison of typical strain noise am- tors, a reduced-order quadrature model of the effective- plitude spectra during the first observing run and early precession waveform [15{18] (the most computationally in the second for both of the LIGO detectors [1]. For the expedient model), and a power spectral density cal- Hanford detector, shot-noise limited performance was im- culated using a parametrized model of the detector proved above about 500 Hz by increasing the laser power. noise [19, 20]. A stretch of 4 s of data, centered on There are new broad mechanical resonance features (e.g., the event, was analysed across a frequency range of 20{ at 150 Hz, 320 Hz and 350 Hz) due to increased beam 1024 Hz. We assumed uninformative prior probabili- pointing∼ jitter from the laser, as well as the coupling ties [11, 13]; technical restrictions of the reduced-order of the jitter to the detector's gravitational-wave channel quadrature required us to limit spin magnitudes to < 0:8 that is larger than in the Livingston detector. The in- and impose cuts on the masses (as measured in the de- det det crease in the noise between 40 Hz and 100 Hz is currently tector frame) such that m1;2 [5:5; 160] M , 2 M 2 under investigation. -
Determining the Hubble Constant with Black Hole Mergers in Active Galactic Nuclei
Determining the Hubble Constant with AGN-assisted Black Hole Mergers Y. Yang,1 V. Gayathri,1 S. M´arka,2 Z. M´arka,2 and I. Bartos1, ∗ 1Department of Physics, University of Florida, PO Box 118440, Gainesville, FL 32611, USA 2Department of Physics, Columbia University in the City of New York, New York, NY 10027, USA Gravitational waves from neutron star mergers have long been considered a promising way to mea- sure the Hubble constant, H0, which describes the local expansion rate of the Universe. While black hole mergers are more abundantly observed, their expected lack of electromagnetic emission and poor gravitational-wave localization makes them less suited for measuring H0. Black hole mergers within the disks of Active Galactic Nuclei (AGN) could be an exception. Accretion from the AGN disk may produce an electromagnetic signal, pointing observers to the host galaxy. Alternatively, the low number density of AGNs could help identify the host galaxy of 1 − 5% of mergers. Here we show that black hole mergers in AGN disks may be the most sensitive way to determine H0 with gravitational waves. If 1% of LIGO/Virgo's observations occur in AGN disks with identified host galaxies, we could measure H0 with 1% uncertainty within five years, likely beyond the sensitivity of neutrons star mergers. I. INTRODUCTION Multi-messenger gravitational-wave observations rep- resent a valuable, independent probe of the expansion of the Universe [1]. The Hubble constant, which de- scribes the rate of expansion, can measured using Type Ia supernovae, giving a local expansion rate of H0 = 74:03 ± 1:42 km s−1 Mpc−1 [2]. -
Advanced Virgo: Status of the Detector, Latest Results and Future Prospects
universe Review Advanced Virgo: Status of the Detector, Latest Results and Future Prospects Diego Bersanetti 1,* , Barbara Patricelli 2,3 , Ornella Juliana Piccinni 4 , Francesco Piergiovanni 5,6 , Francesco Salemi 7,8 and Valeria Sequino 9,10 1 INFN, Sezione di Genova, I-16146 Genova, Italy 2 European Gravitational Observatory (EGO), Cascina, I-56021 Pisa, Italy; [email protected] 3 INFN, Sezione di Pisa, I-56127 Pisa, Italy 4 INFN, Sezione di Roma, I-00185 Roma, Italy; [email protected] 5 Dipartimento di Scienze Pure e Applicate, Università di Urbino, I-61029 Urbino, Italy; [email protected] 6 INFN, Sezione di Firenze, I-50019 Sesto Fiorentino, Italy 7 Dipartimento di Fisica, Università di Trento, Povo, I-38123 Trento, Italy; [email protected] 8 INFN, TIFPA, Povo, I-38123 Trento, Italy 9 Dipartimento di Fisica “E. Pancini”, Università di Napoli “Federico II”, Complesso Universitario di Monte S. Angelo, I-80126 Napoli, Italy; [email protected] 10 INFN, Sezione di Napoli, Complesso Universitario di Monte S. Angelo, I-80126 Napoli, Italy * Correspondence: [email protected] Abstract: The Virgo detector, based at the EGO (European Gravitational Observatory) and located in Cascina (Pisa), played a significant role in the development of the gravitational-wave astronomy. From its first scientific run in 2007, the Virgo detector has constantly been upgraded over the years; since 2017, with the Advanced Virgo project, the detector reached a high sensitivity that allowed the detection of several classes of sources and to investigate new physics. This work reports the Citation: Bersanetti, D.; Patricelli, B.; main hardware upgrades of the detector and the main astrophysical results from the latest five years; Piccinni, O.J.; Piergiovanni, F.; future prospects for the Virgo detector are also presented. -
Searching for the Neutron Star Or Black Hole Resulting from Gw170817
SEARCHING FOR THE NEUTRON STAR OR BLACK HOLE RESULTING FROM GW170817 With the detection of a binary neutron star merger by the Advanced Laser Interferometer Gravitational Wave Observatory (LIGO) and Virgo, a natural question to ask is: what happened to the resulting object that was formed? The merger of two neutron stars can lead to four ultimate outcomes: (i) the prompt formation of a black hole, (ii) the formation of a "hypermassive" neutron star that collapses to a black hole in less than a second, (iii) the formation of a "supramassive" neutron star that collapses to a black hole on much longer timescales, (iv) the formation of a stable neutron star. Which of these four possibilities occurs depends on how much mass remains in the resulting object, as well as the composition and properties of matter inside neutron stars. Knowing the masses of the original two neutron stars before they merged, which can be measured from the gravitational wave signal detected, and under some assumptions about the compactness of neutron stars, it seems most likely that the resulting object was a hypermassive neutron star, although the other options cannot be excluded either. In this analysis, we search for gravitational waves from the post-merger object, and although we do not find anything, we set the groundwork for future searches when we have further improved the sensitivity of our detectors and where we might also observe a merger even closer to us. WHAT MIGHT WE EXPECT TO OBSERVE? Simulations tell us that the remnant object that results from merging binary neutron stars also emits gravitational waves. -
Probing the Nuclear Equation of State from the Existence of a 2.6 M Neutron Star: the GW190814 Puzzle
S S symmetry Article Probing the Nuclear Equation of State from the Existence of a ∼2.6 M Neutron Star: The GW190814 Puzzle Alkiviadis Kanakis-Pegios †,‡ , Polychronis S. Koliogiannis ∗,†,‡ and Charalampos C. Moustakidis †,‡ Department of Theoretical Physics, Aristotle University of Thessaloniki, 54124 Thessaloniki, Greece; [email protected] (A.K.P.); [email protected] (C.C.M.) * Correspondence: [email protected] † Current address: Aristotle University of Thessaloniki, 54124 Thessaloniki, Greece. ‡ These authors contributed equally to this work. Abstract: On 14 August 2019, the LIGO/Virgo collaboration observed a compact object with mass +0.08 2.59 0.09 M , as a component of a system where the main companion was a black hole with mass ∼ − 23 M . A scientific debate initiated concerning the identification of the low mass component, as ∼ it falls into the neutron star–black hole mass gap. The understanding of the nature of GW190814 event will offer rich information concerning open issues, the speed of sound and the possible phase transition into other degrees of freedom. In the present work, we made an effort to probe the nuclear equation of state along with the GW190814 event. Firstly, we examine possible constraints on the nuclear equation of state inferred from the consideration that the low mass companion is a slow or rapidly rotating neutron star. In this case, the role of the upper bounds on the speed of sound is revealed, in connection with the dense nuclear matter properties. Secondly, we systematically study the tidal deformability of a possible high mass candidate existing as an individual star or as a component one in a binary neutron star system. -
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]. -
Measuring the Unknown Forces THAT DRIVE Neutron Star Mergers
Measuring the Unknown Forces THAT DRIVE Neutron Star Mergers Interview with Professor Eliot Quataert Figure 1: Merger of two neutron stars and their corresponding gravitational waves. Modeled after BY CASSIDY HARDIN, MICHELLE the first gravitational waves from a neutron star LEE, AND KAELA SEIERSEN detected by the LIGO telescope.1 Eliot Quataert is a Professor of Astronomy and Physics at the University of California, Berkeley. He is also the director of the Theoretical Astrophysics Center, examining cosmology, planetary dynamics, the interstellar medium, and star and planet formation. Professor Quataert’s specific interests include black holes, stellar physics, and galaxy formation. In this interview, we discuss the formation of neutron stars, the detection of neutron star mergers, and the general-relativistic magnetohydrodynamic (GRMHD) model that was used to predict the behavior of these mergers. Analysis of these cosmic events is significant because it sheds light on the origins of the heavier elements that make up our universe. Professor Eliot Quataert. 42 Berkeley Scientific Journal | FALL 2018 now. It was really getting involved with research that allowed me to realize that I love astrophysics. One of the great things about astrophysics relative to particle or string theory is the close con- nection with observation. This interplay between the abstract, theoretical things I do and the observational side is really fun and exciting, and it also keeps my research grounded in reality. I think this combination is what really convinced me to do astrophysics in graduate school. Right now, I’m working on relating stars with black holes and investigating how stars collapse at the end of their lives. -
Supernova Physics with Gravitational Waves: Newborn Black Holes Are “Kicked”
Supernova physics with gravitational waves: Newborn black holes are “kicked” Richard O’Shaughnessy [email protected] 614 906 9649 Davide Gerosa [email protected] 626 395 6829 Daniel Wysocki [email protected] ! ! Accepted for publication in Physical Review Letters Poster 317.07 [see iPoster] June 5, AAS 2 3 GW151226: Gravitational waves from a black hole binary B. P.• ABBOTTGW151226et al. is the second, less massive binary black hole confidently detectedPHYS. by REV. LIGO X 6, 041015 (2016) GW151226 Abbott et al, PRX 6, 041015 (2016) ; PRL 118 221101 (2017) FIG. 4. Posterior probability densities of the masses, spins, and distance to the three events GW150914, LVT151012, and GW151226. source For the two-dimensional distributions, the contours show 50% and 90% credible regions. Top left panel: Component masses m1 and source source source m2 for the three events. We use the convention that m1 ≥ m2 , which produces the sharp cut in the two-dimensional source 0.3 distribution. For GW151226 and LVT151012, the contours follow lines of constant chirp mass (M 8.9−þ0.3 M and source 1.4 ¼ ⊙ M 15:1−þ1.1 M , respectively). In all three cases, both masses are consistent with being black holes. Top right panel: The mass and¼ dimensionless⊙ spin magnitude of the final black holes. Bottom left panel: The effective spin and mass ratios of the binary components. Bottom right panel: The luminosity distance to the three events. following section and are consistent with our expect- closely mirror the original analysis of GW150914, as ations for an astrophysical BBH source. -
Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: Gw170817 and Grb 170817A
GRAVITATIONAL WAVES AND GAMMA-RAYS FROM A BINARY NEUTRON STAR MERGER: GW170817 AND GRB 170817A The gravitational-wave signal GW170817 was detected on August 17, 2017 by the Advanced LIGO and Virgo observatories. This is the first signal thought to be due to the merger of two neutron stars. Only 1.7 seconds after the gravitational-wave signal was detected, the Fermi Gamma-ray Burst Monitor (GBM) and the Anticoincidence Shield for the SPectrometer for the INTErnational Gamma-Ray Astrophysics Laboratory (INTEGRAL SPI-ACS) detected a short gamma-ray burst GRB 170817A. For decades astronomers suspected that short gamma-ray bursts were produced by the merger of two neutron stars or a neutron star and a black hole. The combination of GW170817 and GRB 170817A provides the first direct evidence that colliding neutron stars can indeed produce short gamma-ray bursts. INTRODUCTION FIGURES FROM THE PUBLICATION Gamma-Ray Bursts (GRBs) are some of the most energetic events For more information on the meaning of these figures, see the full publication here. observed in Nature. They typically release as much energy in just a few seconds as our Sun will throughout its 10 billion-year life. They occur approximately once a day and come from random points on the sky. These GRBs can last anywhere from fractions of seconds to thousands of seconds. However, we usually divide them in two groups based roughly on their duration, with the division being at the 2 second mark (although more sophisticated features are also taken into account in the classification). Long GRBs (>2 seconds) are caused by the core-collapse of rapidly rotating massive stars. -
50 Years of Pulsars: Jocelyn Bell Burnell an Interview P
LIGO Scientific Collaboration Scientific LIGO issue 11 9/2017 LIGO MAGAZINE O2: Third Detection! 10:11:58.6 UTC, 4 January 2017 ELL F, H O L P IS L A E ! Y B D O O G 50 Years of Pulsars: Jocelyn Bell Burnell An interview p. 6 The Search for Continuous Waves To name a neutron star p.10 ... and in 1989: The first joint interferometric observing run p. 26 Before the Merger: Spiraling Black Holes Front cover image: Artist’s conception shows two merging black holes similar to those detected by LIGO. The black holes are spinning in a non-aligned fashion, which means they have different orientations relative to the overall orbital motion of the pair. LIGO found a hint of this phenomenon in at least one black hole of the GW170104 system. Image: LIGO/Caltech/MIT/Sonoma State (Aurore Simonnet) Image credits Front cover main image – Credit: LIGO/Caltech/MIT/Sonoma State (Aurore Simonnet) Front cover inset LISA – Courtesy of LISA Consortium/Simon Barke Front cover inset of Jocelyn Bell Burnell and the 4 acre telescope c 1967 courtesy Jocelyn Bell Burnell. Front cover inset of the supernova remnant G347.3-0.5 – Credit: Chandra: NASA/CXC/SAO/P.Slane et al.; XMM-Newton:ESA/RIKEN/J.Hiraga et al. p. 3 Comic strip by Nutsinee Kijbunchoo p. 4-5 Photos by Matt Gush, Bryce Vickmark and Josh Meister p. 6 Jocelyn Bell Burnell and the 4 acre telescope courtesy Jocelyn Bell Burnell. Paper chart analysis courtesy Robin Scagell p. 8 Pulsar chart recordings courtesy Mullard Radio Astronomy Observatory p. -
Search for Gev Gamma-Ray Counterparts of Gravitational Wave
Draft version July 5, 2018 Typeset using LATEX default style in AASTeX62 Search for GeV Gamma-ray Counterparts of Gravitational Wave Events by CALET O. Adriani,1,2 Y. Akaike,3,4 K. Asano,5 Y. Asaoka,6,7 M.G. Bagliesi,8,9 E. Berti,1,2 G. Bigongiari,8,9 W.R. Binns,10 S. Bonechi,8,9 M. Bongi,1,2 P. Brogi,8,9 J.H. Buckley,10 N. Cannady,11 G. Castellini,12 C. Checchia,13, 14 M.L. Cherry,11 G. Collazuol,13,14 V. Di Felice,15,16 K. Ebisawa,17 H. Fuke,17 T.G. Guzik,11 T. Hams,3,18 M. Hareyama,19 N. Hasebe,6 K. Hibino,20 M. Ichimura,21 K. Ioka,22 W. Ishizaki,5 M.H. Israel,10 K. Kasahara,6 J. Kataoka,6 R. Kataoka,23 Y. Katayose,24 C. Kato,25 N. Kawanaka,26, 27 Y. Kawakubo,28 H.S. Krawczynski,10 J.F. Krizmanic,18,3 K. Kohri,29 T. Lomtadze,9 P. Maestro,8,9 P.S. Marrocchesi,8,9 A.M. Messineo,30,9 J.W. Mitchell,4 S. Miyake,31 A.A. Moiseev,32, 18 K. Mori,6,17 M. Mori,33 N. Mori,2 H.M. Motz,34 K. Munakata,25 H. Murakami,6 S. Nakahira,35 J. Nishimura,17 G.A. de Nolfo,36 S. Okuno,20 J.F. Ormes,37 S. Ozawa,6 L. Pacini,1,12,2 F. Palma,15,16 P. Papini,2 A.V. Penacchioni,8,38 B.F. Rauch,10 S.B. Ricciarini,12,2 K. -
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>