The LIGO Scientific Collaboration
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5 Optical Design
ET-0106A-10 issue :2 ET Design Study date :January27,2011 page :204of315 5 Optical design 5.1 Description Responsible: WP3 coordinator, A. Freise Put here the description of the content of the section . 5.2 Executive Summary Responsible: WP3 coordinator, A. Freise Put here a summary of the main achievement/statements of this section . 5.3 Review on the geometry of the observatory Author(s): Andreas Freise,StefanHild This section briefly reviews the reasoning behind the shape of current gravitational wave detectors and then discusses alternative geometries which can be of interest for third-generation detectors. We will use the ter- minology introduced in the review of a triangular configuration [220] and discriminate between the geometry, topology and configuration of a detector as follows: The geometry describes the position information of one or several interferometers, defined by the number of interferometers, their location and relative orientation. The topology describes the optical system formed by its core elements. The most common examples are the Michelson, Sagnac and Mach–Zehnder topologies. Finally the configuration describes the detail of the optical layout and the set of parameters that can be changed for a given topology, ranging from the specifications of the optical core elements to the control systems, including the operation point of the main interferometer. Please note that the addition of optical components to a given topology is often referred to as a change in configuration. 5.3.1 The L-shape Current gravitational wave detectors represent the most precise instruments for measuring length changes. They are laser interferometers with km-long arms and are operated differently from many precision instruments built for measuring an absolute length. -
LIGO Detector and Hardware Introduction
LIGO Detector and Hardware Introduction Virtual Open Data Workshop May 2020 LIGO-G2000795 Outline • Introduction 45W • Interferometry 40W 1.6kW 200kW Locking Optical cavities • Hardware • Noise Fundamental Technical • Commissioning/Observation Runs • Future Detector Plans • Bibliography Gravitational Waves • Metric tensor perturbation in GR = + 2 polarization in GR Scalar and other possible waves ℎ • Free falling masses • Change in laser propagation time • Phase difference in light ∝ ℎ • Interferometry detects phase difference ∝ ℎ • Astronomical Sources Modeling Modeled Unmodeled /Length Modeled vs Unmodeled Short Inspirals (BBH, Bursts Short vs Long BNS, BH/NS) (Supernova) Long Continuous Waves Stochastic Known vs Unknown (Pulsars) Background Sensitivity Estimate • Strain from single photon: = 10 2 • Need strain 10 � −10 ℎ ≅ • Shot noise SNR− 22 = 10 improvement,∝ � 10 photons At1 1002 Hz equivalent to power24 of 20 MW • • With 200 W of input laser power, 45W 200kW 40W 1.6kW requires power gain of 100,000 Total optical gain in LIGO is ~50,000 Ignores other noise sources Gravitational Wave Detector Network GEO 600: Germany Virgo: Italy KAGRA: Japan Interferometry • Book by Peter Saulson • Michelson interferometer Fringe splitting • Fabry-Perot arms Cavity pole, = ⁄4ℱ • Pound-Drever-Hall locking 45W 200kW 40W 1.6kW Match laser frequency to cavity length RF modulation with EOM • Feedback and controls Other LIGO Cavities • Mode cleaners Input and output 45W 200kW 40W 1.6kW Single Gauss-Laguerre mode • Power recycling Output dark -
The Einstein Telescope (ET) Is a Proposed Underground Infrastructure to Host a Third- Generation, Gravitational-Wave Observatory
The Einstein Telescope (ET) is a proposed underground infrastructure to host a third- generation, gravitational-wave observatory. It builds on the success of current, second-generation laser- interferometric detectors Advanced Virgo and Advanced LIGO, whose breakthrough discoveries of merging black holes (BHs) and neutron stars over the past 5 years have ushered scientists into the new era of gravitational-wave astronomy. The Einstein Telescope will achieve a greatly improved sensitivity by increasing the size of the interferometer from the 3km arm length of the Virgo detector to 10km, and by implementing a series of new technologies. These include a cryogenic system to cool some of the main optics to 10 – 20K, new quantum technologies to reduce the fluctuations of the light, and a set of infrastructural and active noise-mitigation measures to reduce environmental perturbations. The Einstein Telescope will make it possible, for the first time, to explore the Universe through gravitational waves along its cosmic history up to the cosmological dark ages, shedding light on open questions of fundamental physics and cosmology. It will probe the physics near black-hole horizons (from tests of general relativity to quantum gravity), help understanding the nature of dark matter (such as primordial BHs, axion clouds, dark matter accreting on compact objects), and the nature of dark energy and possible modifications of general relativity at cosmological scales. Exploiting the ET sensitivity and frequency band, the entire population of stellar and intermediate mass black holes will be accessible over the entire history of the Universe, enabling to understand their origin (stellar versus primordial), evolution, and demography. -
Seismic Characterization of the Euregio Meuse-Rhine in View of Einstein Telescope
SEISMIC CHARACTERIZATION OF THE EUREGIO MEUSE-RHINE IN VIEW OF EINSTEIN TELESCOPE 13 September 2019 First results of seismic studies of the Belgian-Dutch-German site for Einstein Telescope Soumen Koley1, Maria Bader1, Alessandro Bertolini1, Jo van den Brand1,2, Henk Jan Bulten1,3, Stefan Hild1,2, Frank Linde1,4, Bas Swinkels1, Bjorn Vink5 1. Nikhef, National Institute for Subatomic Physics, Amsterdam, The Netherlands 2. Maastricht University, Maastricht, The Netherlands 3. VU University Amsterdam, Amsterdam, The Netherlands 4. University of Amsterdam, Amsterdam, The Netherlands 5. Antea Group, Maastricht, The Netherlands CONFIDENTIAL Figure 1: Artist impression of the Einstein Telescope gravitational wave observatory situated at a depth of 200-300 meters in the Euregio Meuse-Rhine landscape. The triangular topology with 10 kilometers long arms allows for the installation of multiple so-called laser interferometers. Each of which can detect ripples in the fabric of space-time – the unique signature of a gravitational wave – as minute relative movements of the mirrors hanging at the bottom of the red and white towers indicated in the illustration at the corners of the triangle. 1 SEISMIC CHARACTERIZATION OF THE EUREGIO MEUSE-RHINE IN VIEW OF EINSTEIN TELESCOPE Figure 2: Drill rig for the 2018-2019 campaign used for the completion of the 260 meters deep borehole near Terziet on the Dutch-Belgian border in South Limburg. Two broadband seismic sensors were installed: one at a depth of 250 meters and one just below the surface. Both sensors are accessible via the KNMI portal: http://rdsa.knmi.nl/dataportal/. 2 SEISMIC CHARACTERIZATION OF THE EUREGIO MEUSE-RHINE IN VIEW OF EINSTEIN TELESCOPE Executive summary The European 2011 Conceptual Design Report for Einstein Telescope identified the Euregio Meuse-Rhine and in particular the South Limburg border region as one of the prospective sites for this next generation gravitational wave observatory. -
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]. -
Matters of Gravity
MATTERS OF GRAVITY The newsletter of the Division of Gravitational Physics of the American Physical Society Number 49 June 2017 Contents DGRAV News: we hear that . , by David Garfinkle ..................... 3 DGRAV student travel grants, by Beverly Berger .............. 4 Research Briefs: The Discovery of GW170104, by Jenne Driggers and Salvatore Vitale ... 5 Obituary: Remembering Vishu, by Naresh Dadhich and Bala Iyer ........... 8 Remembering Cecile DeWitt-Morette, by Yvonne Choquet-Bruhat ..... 13 arXiv:1706.06183v2 [gr-qc] 22 Jun 2017 Remembering Larry Shepley, by Richard Matzner and Mel Oakes ...... 15 Remembering Marcus Ansorg, by Bernd Br¨ugmannand Reinhard Meinel . 16 Conference Reports: EGM20, by Abhay Ashtekar ......................... 18 Editor David Garfinkle Department of Physics Oakland University Rochester, MI 48309 Phone: (248) 370-3411 Internet: garfinkl-at-oakland.edu WWW: http://www.oakland.edu/?id=10223&sid=249#garfinkle Associate Editor Greg Comer Department of Physics and Center for Fluids at All Scales, St. Louis University, St. Louis, MO 63103 Phone: (314) 977-8432 Internet: comergl-at-slu.edu WWW: http://www.slu.edu/colleges/AS/physics/profs/comer.html ISSN: 1527-3431 DISCLAIMER: The opinions expressed in the articles of this newsletter represent the views of the authors and are not necessarily the views of APS. The articles in this newsletter are not peer reviewed. 1 Editorial The next newsletter is due December 2017. This and all subsequent issues will be available on the web at https://files.oakland.edu/users/garfinkl/web/mog/ All issues before number 28 are available at http://www.phys.lsu.edu/mog Any ideas for topics that should be covered by the newsletter should be emailed to me, or Greg Comer, or the relevant correspondent. -
A Brief History of Gravitational Waves
Review A Brief History of Gravitational Waves Jorge L. Cervantes-Cota 1, Salvador Galindo-Uribarri 1 and George F. Smoot 2,3,4,* 1 Department of Physics, National Institute for Nuclear Research, Km 36.5 Carretera Mexico-Toluca, Ocoyoacac, Mexico State C.P.52750, Mexico; [email protected] (J.L.C.-C.); [email protected] (S.G.-U.) 2 Helmut and Ana Pao Sohmen Professor at Large, Institute for Advanced Study, Hong Kong University of Science and Technology, Clear Water Bay, 999077 Kowloon, Hong Kong, China. 3 Université Sorbonne Paris Cité, Laboratoire APC-PCCP, Université Paris Diderot, 10 rue Alice Domon et Leonie Duquet 75205 Paris Cedex 13, France. 4 Department of Physics and LBNL, University of California; MS Bldg 50-5505 LBNL, 1 Cyclotron Road Berkeley, CA 94720, USA. * Correspondence: [email protected]; Tel.:+1-510-486-5505 Abstract: This review describes the discovery of gravitational waves. We recount the journey of predicting and finding those waves, since its beginning in the early twentieth century, their prediction by Einstein in 1916, theoretical and experimental blunders, efforts towards their detection, and finally the subsequent successful discovery. Keywords: gravitational waves; General Relativity; LIGO; Einstein; strong-field gravity; binary black holes 1. Introduction Einstein’s General Theory of Relativity, published in November 1915, led to the prediction of the existence of gravitational waves that would be so faint and their interaction with matter so weak that Einstein himself wondered if they could ever be discovered. Even if they were detectable, Einstein also wondered if they would ever be useful enough for use in science. -
A Primer on LIGO and Virgo Gravitational Wave Detectors
A primer on LIGO and Virgo gravitational wave detectors Jo van den Brand, Nikhef and VU University Amsterdam, [email protected] Gravitational Wave Open Data Workshop #2, Paris, April 8, 2019 Interferometric gravitational wave detectors Tiny vibrations in space can now be observed by using the kilometer-scale laser-based interferometers of LIGO and Virgo. This enables an entire new field in science Eleven detections…so far First gravitational wave detection with GW150914 and first binary neutron star GW170817 Event GW150914 Chirp-signal from gravitational waves from two Einsteincoalescing black holes were Telescope observed with the LIGO detectors by the LIGO-Virgo Consortium on September 14, 2015 The next gravitational wave observatory Event GW150914 On September 14th 2015 the gravitational waves generated by a binary black hole merger, located about 1.4 Gly from Earth, crossed the two LIGO detectors displacing their test masses by a small fraction of the radius of a proton Displacement Displacement ( 0.005 0.0025 0.000 Proton radii Proton - 0.0025 - 0.005 ) Proton radius=0.87 fm Measuring intervals must be smaller than 0.01 seconds Laser interferometer detectorsEinstein Telescope The next gravitational wave observatory Laser interferometer detectorsEinstein Telescope The next gravitational wave observatory LIGO Hanford VIRGO KAGRA LIGO Livingston GEO600 Effect of a strong gravitational wave on ITF arm 2Δ퐿 h= = 10−22 퐿 Laser interferometer detectors Michelson interferometer If we would use a single photon and only distinguish between bright and dark fringe, then such an ITF would not be sensitive: −6 휆/2 0.5 ×10 m −10 ℎcrude ≈ = ≈ 10 퐿optical 4000 m Need to do 1012 times better. -
The Virgo Interferometer
The Virgo Interferometer www.virgo-gw.eu THE VIRGO INTERFEROMETER Located near the city of Pisa in Italy, the Virgo interferometer is the most sensitive gravitational wave detector in Europe. The latest version of the interferometer – the Advanced Virgo – was built in 2012, and has been operational since 2017. Virgo is part of a scientific collaboration of more than 100 institutes from 10 European countries. By detecting and analysing gravitational wave signals, which arise from collisions of black holes or neutron stars millions of lightyears away, Virgo’s goal is to advance our understanding of fundamental physics, astronomy and cosmology. In this exclusive interview, we speak with the spokesperson of the Virgo Collaboration, Dr Jo van den Brand, who discusses Virgo’s achievements, plans for the future, and the fascinating field of gravitational wave astronomy. In February 2016, alongside LIGO, the Virgo Collaboration announced the first direct observation of gravitational waves, made using the Advanced LIGO detectors. Please tell us about the excitement amongst members of Collaboration, and what this discovery meant for Virgo. The discovery of gravitational waves from the merger of two black holes was a great achievement and caused excitement to almost all impassioned scientists. The merger was the most powerful event ever detected and could only be observed with gravitational waves. We showed once and for all that spacetime is a dynamical quantity, and we provided the first direct evidence for CREDIT: EGO/Virgo the existence of black holes. Moreover, we detected the collision and How are observable gravitational The curvature fluctuations are tiny and subsequent coalescence of two black waves generated? cause minor relative length differences. -
Stefan W. Ballmer
Stefan W. Ballmer Curriculum Vitae Department of Physics Phone: +1-315-443-3882 Syracuse University Cell: +1-315-278-1154 Syracuse, NY 13244 Fax: +1-315-443-9103 USA E-mail: [email protected] Citizenship: USA, Switzerland Web: thecollege.syr.edu/people/faculty/ballmer-stefan RECENT AND CURRENT POSITIONS Jun 2016 - Associate Professor of Physics present Syracuse University, Syracuse, NY May 2019 - Visiting Associate Professor of Physics Jun 2019 Institute for Cosmic Ray Research, University of Tokyo, Japan May 2018 - Visiting Associate Professor of Physics Jun 2018 Institute for Cosmic Ray Research, University of Tokyo, Japan May 2017 - Visiting Associate Professor of Physics Jun 2017 University of Tokyo, Japan Jun 2013 - Research leave at the LIGO Hanford Observatory Aug 2014 Commissioning the Advanced LIGO interferometer Aug 2010 - Assistant Professor of Physics May 2016 Syracuse University, Syracuse, NY Dec 2009 - NAOJ Visiting Researcher Aug 2010 National Astronomical Observatory of Japan. Sep 2009 - JSPS Postdoctoral Fellow (Gaikokujin Tokubetsu Kenkyuin) Nov 2009 National Astronomical Observatory of Japan. Jul 2006 - Robert A. Millikan Postdoctoral Fellow Aug 2009 California Institute of Technology, Pasadena, CA EDUCATION Jun 2006 Ph.D. Physics, Massachusetts Institute of Technology (MIT), Cambridge, MA Experimental Astrophysics, Laser Interferometer Gravitational Wave Observatory (LIGO). Apr 2000 Diploma (equivalent to Master of Science), Physics, Swiss Federal Institute of Technology (ETH) Zurich, Switzerland With honor, in Theoretical -
Joshua R. Smith
Joshua R. Smith The Nicholas and Lee Begovich Center for Gravitational-Wave Physics and Astronomy Department of Physics California State University Fullerton 800 N. State College Blvd. Fullerton, CA 92831 E-mail: [email protected] Phone: (657)-278-3716 Web: https://physics.fullerton.edu/∼josmith/ Appointments 2016– Dan Black Director of Gravitational-Wave Physics and Astronomy 2018– Professor of Physics 2014–2018 Associate Professor of Physics 2010–2014 Assistant Professor of Physics California State University Fullerton (CSUF) 2007–2009 Postdoctoral Research Associate in Physics Syracuse University 2006–2007 Postdoctoral Fellow in Physics Albert Einstein Institute Hannover / EGO-Virgo Education 2002–2006 Ph.D. Physics (Dr. rer. nat.), Leibniz Universitat¨ Hannover • Advisor: Karsten Danzmann • Thesis: “Formulation of Instrument Noise Analysis Techniques and Their Use in the Commissioning of the Gravitational Wave Observatory GEO 600” 1998–2002 B.Sc. Physics, Syracuse University • Advisor: Peter Saulson • Thesis: “Thermal Noise Associated with Silicate Bonding” Leadership 2012– Director, The Nicholas and Lee Begovich Center for Gravitational-Wave Physics and Astron- omy, CSUF 2019– Co-I, Cosmic Explorer Project, Member, Cosmic Explorer Consortium 2016–2017 Member, Executive Committee, APS Far West Section 2011–2015 Chair, Detector Characterization Group, LIGO Scientific Collaboration 2011–2015 Member, Executive Committee, LIGO Scientific Collaboration 2008– Member, Council, LIGO Scientific Collaboration 2008–2010 Co-chair, Glitch Working -
A Brief History of LIGO
A Brief History of LIGO One hundred years ago, using his recently formulated general relativity theory, Albert Einstein predicted the existence of gravitational waves and described their properties. To Einstein these waves seemed too weak ever to be detected, even for the strongest sources that he could conceive. Over the subsequent decades, our improving knowledge of the universe (black holes, neutron stars, supernovae …) and the march of technology (lasers, computers, solid state electronics, low loss optics….) have changed that. In the 1960s, Joseph Weber at the University of Maryland pioneered the effort to build detectors for gravitational waves, using large cylinders of aluminum that vibrate in response to a passing wave, an approach which broke the ground for the field of gravitational-wave searches. LIGO’s approach, using laser interferometry to monitor the relative motion of freely hanging mirrors, was proposed as a theoretical concept form in 1962 by Michael Gertsenshtein and Vladislav Pustovoit in Moscow Russia, and independently several years later by Weber and by Rainer Weiss in America. In 1967, Weiss investigated a laser interferometer limited at some frequencies by quantum shot noise, and in 1972 he completed the invention of the interferometric gravitational wave detector by identifying all the fundamental noise sources that such a detector must face, and conceiving ways to deal with each of them, and by showing that — at least in principle — these ways could lead to detector sensitivities good enough to detect waves from astrophysical sources. Prototype interferometric gravitational wave detectors (“interferometers”) were built in the late 1960s by Robert Forward and colleagues at Hughes Research Laboratories (with mirrors mounted on a vibration isolated plate rather than free swinging), and in the 1970s (with free swinging mirrors between which light bounced many times) by Weiss at MIT, and then by Hans Billing and colleagues in Garching Germany, and then by Ronald Drever, James Hough and colleagues in Glasgow Scotland.