LIGO Magazine Issue #12 !
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A Time of Great Growth
Newsletter | Spring 2019 A Time of Great Growth Heartfelt greetings from the UC Riverside Department of Physics and Astronomy. This is our annual newsletter, sent out each Spring to stay connected with our former students, retired faculty, and friends in the wider community. The Department continues to grow, not merely in size but also in stature and reputation. For the 2018-2019 academic year, we were pleased to welcome two new faculty: Professors Thomas Kuhlman and Barry Barish. Professor Kuhlman was previously on the faculty at the University of Illinois at Urbana-Champaign. He joins our efforts in the emerging field of biophysics. His research lies in the quantitative imaging and theoretical modeling of biological systems. He works on genome dynamics, quantification of the activity of transposable elements in living cells, and applications to the engineering of genome editing. Professor Barry Barish, who joins us from Caltech, is the winner of the 2017 Nobel Prize in Physics. He brings great prestige to our Department. Along with Professor Richard Schrock of the Department of Chemistry, who also joined UCR in 2018, UCR now has two Nobel Prize winners on its faculty. Professor Barish is an expert on the detection and physics of gravitational waves. He has been one of the key figures in the conception, construction, and operation of the LIGO detector, where gravitational waves were first discovered in 2015, and which led to his Nobel Prize. He is a member of the National Academy of Sciences and the winner of many other prestigious awards. The discovery of gravitational waves is one of the most exciting developments in physics so far this century. -
Arxiv:2007.09714V1 [Gr-Qc] 19 Jul 2020 Tem PSR J0737-3039A/B
Probing Noncommutative Gravity with Gravitational Wave and Binary Pulsar Observations Leah Jenks,1 Kent Yagi,2 and Stephon Alexander1 1Brown Theoretical Physics Center and Department of Physics, Brown University, 182 Hope Street, Providence, Rhode Island, 02903 2Department of Physics, University of Virginia, P.O. Box 400714, Charlottesville, VA 22904-4714, USA (Dated: July 21, 2020) Noncommutative gravity is a natural method of quantizing spacetime by promoting the spacetime coordinates themselves to operators which do not commute. This approach is motivated, for exam- ple, from a quantum gravity perspective, among others. Noncommutative gravity has been tested against the binary black hole merger event GW150914. Here, we extend and improve upon such a previous analysis by (i) relaxing an assumption made on the preferred direction due to noncommuta- tivity, (ii) using posterior samples produced by the LIGO/Virgo Collaborations, (iii) consider other gravitational wave events, namely GW151226, GW170608, GW170814 and GW170817, and (iv) consider binary pulsar observations. Using Kepler's law that contains the noncommutative effect at second post-Newtonian order, we derive corrections to the gravitational waveform phase and the pericenter precession. Using the gravitational wave and double pulsar binary observations, we find bounds on a space-time noncommutative tensor θ0i in terms of the preferred frame direction with respect to the orientation of each binary. We find that the gravitational wave bounds are stronger than the binary pulsar one by an order of magnitude and the noncommutative tensor normalized by the Planck length and time is constrained to be of order unity. I. INTRODUCTION of noncommutative gravity stems from these theories. -
Ripples in Spacetime
editorial Ripples in spacetime The 2017 Nobel prize in Physics has been awarded to Rainer Weiss, Barry C. Barish and Kip S. Thorne “for decisive contributions to the LIGO detector and the observation of gravitational waves”. It is, frankly, difficult to find something original to say about the detection of gravitational waves that hasn’t been said already. The technological feat of measuring fluctuations in the fabric of spacetime less than one-thousandth the width of an atomic nucleus is quite simply astonishing. The scientific achievement represented by the confirmation of a century-old prediction by Albert Einstein is unique. And the collaborative effort that made the discovery possible — the Laser Interferometer Gravitational-Wave Observatory (LIGO) — is inspiring. Adapted from Phys. Rev. Lett. 116, 061102 (2016), under Creative Commons Licence. Rainer Weiss and Kip Thorne were, along with the late Ronald Drever, founders of the project that eventually became known Barry Barish, who was the director Last month we received a spectacular as LIGO. In the 1960s, Thorne, a black hole of LIGO from 1997 to 2005, is widely demonstration that talk of a new era expert, had come to believe that his objects of credited with transforming it into a ‘big of gravitational astronomy was no interest should be detectable as gravitational physics’ collaboration, and providing the exaggeration. Cued by detections at LIGO waves. Separately, and inspired by previous organizational structure required to ensure and Virgo, an interferometer based in Pisa, proposals, Weiss came up with the first it worked. Of course, the passion, skill and Italy, more than 70 teams of researchers calculations detailing how an interferometer dedication of the thousand or so scientists working at different telescopes around could be used to detect them in 1972. -
Kilonovae and Short Hard Bursts A.K.A: Electromagnetic Counterparts to Gravitational Waves
Kilonovae and short hard bursts a.k.a: electromagnetic counterparts to gravitational waves Igor Andreoni for the Multi-Messenger Astronomy working group ZTF Phase II: NSF reverse site visit November 19th 2020 Electromagnetic counterparts to gravitational waves Short hard GRB - Are neutron star mergers the dominant sites for heavy element nucleosynthesis? - What extreme Physics can we learn? Kilonova (optical/IR) - How can we use kilonovae for cosmology? - What is the rate of binary neutron Gravitational star and neutron star-black hole mergers? Waves Image credit: NASA November 19th 2020 Igor Andreoni Finding kilonovae is challenging! Kilonovae are rare, fast and faint transients compared to supernovae Faint Fast modified from Andreoni+2018, LSST White Paper November 19th 2020 Igor Andreoni Why do we need ZTF? During the second LIGO-Virgo observing run (O2), the binary neutron star merger GW170817 was localized to 32 deg2 GW170817 (a couple of ZTF pointings) During O3 (2019-2020), the median localization for neutron star mergers was 4,480 deg2! …and the sources were more distant November 19th 2020 Igor Andreoni Gravitational Wave follow-up during O3 We used ZTF to follow-up 15 GW triggers that included at least one neutron star Kilonova luminosity function Kasliwal et al., ApJ, in press Second binary NS merger follow-up Coughlin et al., ApJ Letters, Vol 885, Issue 1, article id. L19, 13 pp. Constraints on NS-BH merger Anand & Coughlin et al., Nature Astronomy, in press November 19th 2020 Igor Andreoni Short, hard gamma-ray bursts (GRBs) We used ZTF to follow-up 8 short GRBs found by the Fermi satellite Ahumada et al., in prep. -
Timing Behavior of the Magnetically Active Rotation-Powered Pulsar in the Supernova Remnant Kesteven 75
https://ntrs.nasa.gov/search.jsp?R=20090038692 2019-08-30T08:05:59+00:00Z View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by NASA Technical Reports Server Timing Behavior of the Magnetically Active Rotation-Powered Pulsar in the Supernova Remnant Kesteven 75 Margaret A. Livingstone 1 , Victoria M. Kaspi Department of Physics, Rutherford Physics Building, McGill University, 3600 University Street, Montreal, Quebec, H3A 2T8, Canada and Fotis. P. Gavriil NASA Goddard Space Flight Center, Astrophysics Science Division, Code 662, Greenbelt, MD 20771 Center for Research and Exploration in Space Science and Technology, University of Maryland Baltimore County, 1000 Hilltop Circle, Baltimore, MD 21 250 ABSTRACT We report a large spin-up glitch in PSR J1846-0258 which coincided with the onset of magnetar-like behavior on 2006 May 31. We show that the pul- sar experienced an unusually large glitch recovery, with a recovery fraction of Q = 5.9 ± 0.3, resulting in a net decrease of the pulse frequency. Such a glitch recovery has never before been observed in a rotation-powered pulsar, however, similar but smaller glitch over-recovery has been recently reported in the magne- tar AXP 4U 0142+61 and may have occurred in the SGR 1900+14. We discuss the implications of the unusual timing behavior in PSR J1846-0258 on its status as the first identified magnetically active rotation-powered pulsar. Subject headings: pulsars: general—pulsars: individual (PSR J1846-0258)—X- rays: stars 1. Introduction PSR J1846-0258 is a. young (-800 yr), 326 ms pulsar, discovered in 2000 with the Rossi X-ray Timing Explorer (RXTE; Gotthelf et al. -
The History of Lasers at Stanford Group
Lasers at 50: Byer The History of Lasers at Stanford Group Robert L. Byer Applied Physics Stanford University [email protected] Abstract In the fifty years since the demonstration of the laser, coherent light has changed the way we work, communicate and play. The generation and control of light is critical for meeting important challenges of the 21st century from fundamental science to the generation of energy. A look back at the early days of the laser at Stanford will be contrasted to the recent breakthroughs in solid state lasers and the applications to fundamental science of gravitational wave detection, remote sensing, and laser induced fusion for energy production. Stanford Historical Society 34th Annual Meeting & Reception May 25, 2010 The History of Lasers at Stanford May 25 2010 Cubberley Auditorium, Staford Byer California – Leader in advanced telescopes for astronomy Group Lick 36 inch refractor The Mount Wilson 100 inch The Palomar 200 inch 1888 1917 1948 The History of Lasers at Stanford May 25 2010 Cubberley Auditorium, Staford From Maser to Laser – stimulated emission at optical frequencies Byer proposed in 1958 – A. Schawlow and C. H. Townes Group The History of Lasers at Stanford May 25 2010 Cubberley Auditorium, Staford Early advances in lasers --- Byer 2009 a Special Year Group Concept of Optical Maser Schawlow & Townes 1958 Ruby Laser Ted Maiman 1960 Nobel Prize awarded in 1964 Townes, Prokhorov and Basov Hg+ Ion Laser Earl Bell 1965 Argon Ion Laser Bill Bridges Tunable cw parametric Laser Harris 1968 Diode bar 1Watt -
Continuous Gravitational Waves from Neutron Stars: Current Status and Prospects
Continuous gravitational waves from neutron stars: current status and prospects Magdalena Sieniawska∗1 and Michał Bejger1 1Nicolaus Copernicus Astronomical Center, Polish Academy of Sciences, Bartycka 18, 00–716 Warszawa, Poland Abstract Gravitational waves astronomy allows us to study objects and events invisi- ble in electromagnetic waves. It is crucial to validate the theories and models of the most mysterious and extreme matter in the Universe: the neutron stars. In addition to inspirals and mergers of neutrons stars, there are currently a few pro- posed mechanisms that can trigger radiation of long-lasting gravitational radiation from neutron stars, such as e.g., elastically and/or magnetically driven deforma- tions: mountains on the stellar surface supported by the elastic strain or magnetic field, free precession, or unstable oscillation modes (e.g., the r-modes). The as- trophysical motivation for continuous gravitational waves searches, current LIGO and Virgo strategies of data analysis and prospects are reviewed in this work. 1 Introduction Gravitational-wave (GW) astronomy has been one of the fastest-growing fields in astro- physics since the first historical detection of a binary black-hole (BH) system GW150814 (Abbott et al., 2016a). In addition to studying the nature of gravitation itself, it may be used to infer information about the astrophysical sources emitting the GWs. This re- view concentrates on a specific kind of prospective GWs: persistent (continuous) grav- itational waves (CGWs), emitted by neutron stars (NSs). The article is arranged as follows. Section1 gathers introductory material: Section 1.1 presents the basics of the GWs theory, Section 1.2 contains a brief overview of GWs detections, Section 1.3 de- arXiv:1909.12600v2 [astro-ph.HE] 5 Nov 2019 scribes properties of NSs and features of hitherto detected NSs-related GWs—a binary NS merger GW170817 (Abbott et al., 2017d), Section 1.4 gathers general information about CGWs, whereas Section 1.5 is devoted to the main data analysis methods used in CGWs searches. -
Search for Electron-Antineutrinos Associated with Gravitational-Wave Events GW150914, GW151012, GW151226, GW170104, GW170608, GW170814, and GW170817 at Daya Bay*
Chinese Physics C Vol. 45, No. 5 (2021) 055001 Editors′ Suggestion Search for electron-antineutrinos associated with gravitational-wave events GW150914, GW151012, GW151226, GW170104, GW170608, GW170814, and GW170817 at Daya Bay* F. P. An1 A. B. Balantekin2 H. R. Band3 M. Bishai4 S. Blyth5 G. F. Cao6 J. Cao6 J. F. Chang6 Y. Chang7 H. S. Chen6 S. M. Chen8 Y. Chen9,10 Y. X. Chen11 J. Cheng6 Z. K. Cheng10 J. J. Cherwinka2 M. C. Chu12 J. P. Cummings13 O. Dalager14 F. S. Deng15 Y. Y. Ding6 M. V. Diwan4 T. Dohnal16 J. Dove17 M. Dvořák16 D. A. Dwyer18 J. P. Gallo19 M. Gonchar20 G. H. Gong8 H. Gong8 W. Q. Gu4 J. Y. Guo10 L. Guo8 X. H. Guo21 Y. H. Guo22 Z. Guo8 R. W. Hackenburg4 S. Hans4,* M. He6 K. M. Heeger3 Y. K. Heng6 A. Higuera23 Y. K. Hor10 Y. B. Hsiung5 B. Z. Hu5 J. R. Hu6 T. Hu6 Z. J. Hu10 H. X. Huang24 X. T. Huang25 Y. B. Huang26 P. Huber27 D. E. Jaffe4 K. L. Jen28 X. L. Ji6 X. P. Ji4 R. A. Johnson29 D. Jones30 L. Kang31 S. H. Kettell4 S. Kohn32 M. Kramer18,32 T. J. Langford3 J. Lee18 J. H. C. Lee33 R. T. Lei31 R. Leitner16 J. K. C. Leung33 F. Li6 J. J. Li8 Q. J. Li6 S. Li31 S. C. Li27 W. D. Li6 X. N. Li6 X. Q. Li34 Y. F. Li6 Z. B. Li10 H. Liang15 C. J. Lin18 G. L. Lin28 S. Lin31 J. J. Ling10 J. M. Link27 L. Littenberg4 B. -
Glitches in Superfluid Neutron Stars
GLITCHES IN SUPERFLUID NEUTRON STARS Marco Antonelli [email protected] Centrum Astronomiczne im. Mikołaja Kopernika Polskiej Akademii Nauk Quantum Turbulence: Cold Atoms, Heavy Ions ans Neutron Stars INT, Seattle (WA) – April 16, 2019 Outline Summary: Why glitches (in radio pulsars) tell us something about rotating neutron stars? - A bit of hystory: why superfluidity is needed to explain glitches. Intrinsic difficulty: model the exchange of angular momentum that causes the glitch (mutual friction) - Many-scales (coherence length → stellar radius) - Possible memory effects (also observed in He-II experiments) Which microscopic input do we need? I will focus on two quantities: - Pinning forces (or better, the critical current for unpinning) - Entrainment Is it possible to use glitches to obtain “model-independent” statements about neutron stars interiors? SPOILER: yes, we have at the moment 2 models: 1 – Activity test → “entrainment” 2 – Largest glitch test → “pinning forces” Question: is it possible to go beyond these two tests? What can be done? Neutron stars – RPPs What we observe, since: What we think it is, since: Hewish, Bell et al., Observation of a rapidly pulsating Pacini, Energy emission from a neutron star (1967) radio source (1968) Gold, Rotating neutron stars as the origin of the pulsating radio sources (1968) Magnetic field lines Radiation beam Coordinated observations with three telescopes: 22-s data slice of the pulsed radiation at four different radio Open issue: precise description bands obtained of the 1.2 s pulsar B1113+16. of beamed emission mechanism Why? Coherent (i.e. non-thermal) emission + brightness + small period: only possible for very compact objects A vibrating WD or NS? excluded by pulsar-timing data: P increases with time. -
On the Single-Event-Based Identification of Primordial Black Hole Mergers at Cosmological Distances
On the single-event-based identification of primordial black hole mergers at cosmological distances Ken K. Y. Ng,1, 2, 3, ∗ Shiqi Chen,1, 2, 3 Boris Goncharov,4, 5 Ulyana Dupletsa,4, 5 Ssohrab Borhanian,6, 7 Marica Branchesi,4, 5 Jan Harms,4, 5 Michele Maggiore,8 B. S. Sathyaprakash,6, 9, 10 and Salvatore Vitale1, 2, 3 1LIGO, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA 2Kavli Institute for Astrophysics and Space Research, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA 3Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA 4Gran Sasso Science Institute (GSSI), I-67100 L'Aquila, Italy 5INFN, Laboratori Nazionali del Gran Sasso, I-67100 Assergi, Italy 6Institute for Gravitation and the Cosmos, Department of Physics, Pennsylvania State University, University Park, PA, 16802, USA 7Theoretisch-Physikalisches Institut, Friedrich-Schiller-Universit¨atJena, 07743, Jena, Germany 8D´epartement de Physique Th´eoriqueand Center for Astroparticle Physics, Universit´ede Gen`eve,24 quai Ansermet, CH{1211 Gen`eve4, Switzerland 9Department of Astronomy & Astrophysics, Pennsylvania State University, University Park, PA, 16802, USA 10School of Physics and Astronomy, Cardiff University, Cardiff, UK, CF24 3AA (Dated: September 14, 2021) The existence of primordial black holes (PBHs), which may form from the collapse of matter overdensities shortly after the Big Bang, is still under debate. Among the potential signatures of PBHs are gravitational waves (GWs) emitted from binary black hole (BBH) mergers at redshifts z & 30, where the formation of astrophysical black holes is unlikely. Future ground-based GW detectors, Cosmic Explorer and Einstein Telescope, will be able to observe equal-mass BBH mergers with total mass of O(10 − 100) M at such distances. -
Instruction Manual Meade Instruments Corporation
Instruction Manual 7" LX200 Maksutov-Cassegrain Telescope 8", 10", and 12" LX200 Schmidt-Cassegrain Telescopes Meade Instruments Corporation NOTE: Instructions for the use of optional accessories are not included in this manual. For details in this regard, see the Meade General Catalog. (2) (1) (1) (2) Ray (2) 1/2° Ray (1) 8.218" (2) 8.016" (1) 8.0" Secondary 8.0" Mirror Focal Plane Secondary Primary Baffle Tube Baffle Field Stops Correcting Primary Mirror Plate The Meade Schmidt-Cassegrain Optical System (Diagram not to scale) In the Schmidt-Cassegrain design of the Meade 8", 10", and 12" models, light enters from the right, passes through a thin lens with 2-sided aspheric correction (“correcting plate”), proceeds to a spherical primary mirror, and then to a convex aspheric secondary mirror. The convex secondary mirror multiplies the effective focal length of the primary mirror and results in a focus at the focal plane, with light passing through a central perforation in the primary mirror. The 8", 10", and 12" models include oversize 8.25", 10.375" and 12.375" primary mirrors, respectively, yielding fully illuminated fields- of-view significantly wider than is possible with standard-size primary mirrors. Note that light ray (2) in the figure would be lost entirely, except for the oversize primary. It is this phenomenon which results in Meade 8", 10", and 12" Schmidt-Cassegrains having off-axis field illuminations 10% greater, aperture-for-aperture, than other Schmidt-Cassegrains utilizing standard-size primary mirrors. The optical design of the 4" Model 2045D is almost identical but does not include an oversize primary, since the effect in this case is small. -
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].