Properties of the Binary Neutron Star Merger GW170817
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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. -
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. -
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]. -
Rotational Glitches in Radio Pulsars and Magnetars
UvA-DARE (Digital Academic Repository) Rotational glitches in radio pulsars and magnetars Antonopoulou, D. Publication date 2015 Document Version Final published version Link to publication Citation for published version (APA): Antonopoulou, D. (2015). Rotational glitches in radio pulsars and magnetars. General rights It is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), other than for strictly personal, individual use, unless the work is under an open content license (like Creative Commons). Disclaimer/Complaints regulations If you believe that digital publication of certain material infringes any of your rights or (privacy) interests, please let the Library know, stating your reasons. In case of a legitimate complaint, the Library will make the material inaccessible and/or remove it from the website. Please Ask the Library: https://uba.uva.nl/en/contact, or a letter to: Library of the University of Amsterdam, Secretariat, Singel 425, 1012 WP Amsterdam, The Netherlands. You will be contacted as soon as possible. UvA-DARE is a service provided by the library of the University of Amsterdam (https://dare.uva.nl) Download date:06 Oct 2021 Rotational glitches in radio pulsars and magnetars ACADEMISCH PROEFSCHRIFT ter verkrijging van de graad van doctor aan de Universiteit van Amsterdam op gezag van de Rector Magnificus prof. dr. D. C. van den Boom ten overstaan van een door het college voor promoties ingestelde commissie, in het openbaar te verdedigen in de Agnietenkapel op woensdag 21 januari 2015, te 14:00 uur door Danai Antonopoulou geboren te Athene, Griekenland Promotiecommissie Promotor: prof. -
Study of Pulsar Wind Nebulae in Very-High-Energy Gamma-Rays with H.E.S.S
Study of Pulsar Wind Nebulae in Very-High-Energy gamma-rays with H.E.S.S. Michelle Tsirou To cite this version: Michelle Tsirou. Study of Pulsar Wind Nebulae in Very-High-Energy gamma-rays with H.E.S.S.. As- trophysics [astro-ph]. Université Montpellier, 2019. English. NNT : 2019MONTS096. tel-02493959 HAL Id: tel-02493959 https://tel.archives-ouvertes.fr/tel-02493959 Submitted on 28 Feb 2020 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. THÈSE POUR OBTENIR LE GRADE DE DOCTEUR DE L’UNIVERSITÉ DE MONTPELLIER En Astrophysiques École doctorale I2S Unité de recherche UMR 5299 Study of Pulsar Wind Nebulae in Very-High-Energy gamma-rays with H.E.S.S. Présentée par Michelle TSIROU Le 17 octobre 2019 Sous la direction de Yves A. GALLANT Devant le jury composé de Elena AMATO, Chercheur, INAF - Acetri Rapporteur Arache DJANNATI-ATAȈ, Directeur de recherche, APC - Paris Examinateur Yves GALLANT, Directeur de recherche, LUPM - Montpellier Directeur de thèse Marianne LEMOINE-GOUMARD, Chargée de recherche, CENBG - Bordeaux Rapporteur Alexandre MARCOWITH, Directeur de recherche, LUPM - Montpellier Président du jury Study of Pulsar Wind Nebulae in Very-High-Energy gamma-rays with H.E.S.S.1 Michelle Tsirou 1High Energy Stereoscopic System To my former and subsequent selves, may this wrenched duality amalgamate ultimately. -
The Glitch Activity of Neutron Stars J
A&A 608, A131 (2017) Astronomy DOI: 10.1051/0004-6361/201731519 & c ESO 2017 Astrophysics The glitch activity of neutron stars J. R. Fuentes1, C. M. Espinoza2, A. Reisenegger1, B. Shaw3, B. W. Stappers3, and A. G. Lyne3 1 Instituto de Astrofísica, Pontificia Universidad Católica de Chile, Av. Vicuña Mackenna 4860, 7820436 Macul, Santiago, Chile e-mail: [email protected] 2 Departamento de Física, Universidad de Santiago de Chile, Avenida Ecuador 3493, 9170124 Estación Central, Santiago, Chile 3 Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, The University of Manchester, Manchester M13 9PL, UK Received 6 July 2017 / Accepted 3 October 2017 ABSTRACT We present a statistical study of the glitch population and the behaviour of the glitch activity across the known population of neutron stars. An unbiased glitch database was put together based on systematic searches of radio timing data of 898 rotation-powered pulsars obtained with the Jodrell Bank and Parkes observatories. Glitches identified in similar searches of 5 magnetars were also included. The database contains 384 glitches found in the rotation of 141 of these neutron stars. We confirm that the glitch size distribution is at least bimodal, with one sharp peak at approximately 20 µHz, which we call large glitches, and a broader distribution of smaller glitches. We also explored how the glitch activityν ˙g, defined as the mean frequency increment per unit of time due to glitches, correlates with the spin frequency ν, spin-down rate jν˙j, and various combinations of these, such as energy loss rate, magnetic field, and spin-down age. -
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. -
Magnetars: Pion Condensates in the Sky?
Magnetars: Pion Condensates in the Sky? N.D. Hari Dass TIFR-TCIS, Hyderabad In collaboration with V. Soni(Jamia) & Dipankar Bhattacharya(IUCAA) IWARA 2018, Ollantaytambo, Peru. N.D. Hari Dass Magnetars & Pion Condensates Some References N.D. Hari Dass and V. Soni, Mon. Not. Royal Astron. Soc., 425, 1558-1566 (2012). H.B. Nielsen and V. Soni, Phys. Lett. B726, 41-44 (2013). N.D. Hari Dass Magnetars & Pion Condensates Neutron Stars Nuclear density ρ 2:8 1014gm=cm3. Equivalently 0 ' n 0:17nucleons=fermi3. 0 ' Stable neutron stars can have masses in the range 0.1 solar mass to 2 solar masses. Most observed pulsars have masses about 1.4 solar masses. Neutron stars produced in core collapse are expected with this mass. Heavier neutron stars are believed to be as a result of acretion later on. Typical radii of NS are 10 - 20 kms. Neutron stars can be thought of as giant nuclei with A 1057! ' N.D. Hari Dass Magnetars & Pion Condensates Neutron Star Structure Density ρ decreases as one moves outwards from the centre. The outer kilometre or so is the Crust. It consists of a lattice of bare nuclei and a degenerate electron gas. Next to the crust is a superfluid layer and vortices here contribute to the angular momentum of the star. These vortices also play an important role in the so called glitches whence the star actually speeds up. The least understood part is the core of the NS. Density here can be in the range of 3-10 times nuclear density. It is also very hot. -
Statistical Properties of the Repeating Fast Radio Burst Source FRB 121102
ISSN: 2641-886X International Journal of Cosmology, Astronomy and Astrophysics Research Article Open Access Statistical properties of the repeating fast radio burst source FRB 121102 Bing Li1-3*, Long-Biao Li4, Zhi-Bin Zhang5, Jin-Jun Geng1,6, Li-Ming Song2,3, Yong-Feng Huang1,6* and Yuan-Pei Yang7,8 1School of Astronomy and Space Science, Nanjing University, Nanjing 210023, China 2Laboratory for Particle Astrophysics, Institute of High Energy Physics, Beijing 100049, China 3Key Laboratory of Particle Astrophysics, Chinese Academy of Sciences, Beijing 100049, China 4School of Mathematics and Physics, Hebei University of Engineering, Handan 056005, China 5College of Physics and Engineering, Qufu Normal University, Qufu 273165, China 6Key Laboratory of Modern Astronomy and Astrophysics (Nanjing University), Ministry of Education, China 7Kavli Institute for Astronomy and Astrophysics, Peking University, Beijing 100871, China 8National Astronomical Observatories, Chinese Academy of Sciences, Beijing 100012, China Article Info Abstract *Corresponding authors: Currently, FRB 121102 is the only fast radio burst source that was observed to give Bing Li out bursts repeatedly. It shows a high repeating rate, with more than one hundred bursts School of Astronomy and Space Science Nanjing University being spotted, but with no obvious periodicity in the activities. Thanks to its repetition, Nanjing 210023, China the source was well localized with a subarcsecond accuracy, leading to a red shift E-mail: [email protected] measurement of about 0.2. FRB 121102 is a unique source that can help us understand Yong-Feng Huang the enigmatic nature of fast radio bursts. In this study, we analyze the characteristics of Professor the waiting times between bursts from FRB 121102. -
GW170814 : a Three-Detector Observation of Gravitational Waves from a Binary Black Hole Coalescence
GW170814 : A three-detector observation of gravitational waves from a binary black hole coalescence The LIGO Scientific Collaboration and The Virgo Collaboration On August 14, 2017 at 10:30:43 UTC, the Advanced Virgo detector and the two Advanced LIGO detectors coherently observed a transient gravitational-wave signal produced by the coalescence of two < stellar mass black holes, with a false-alarm-rate of ∼ 1 in 27 000 years. The signal was observed with a three-detector network matched-filter signal-to-noise ratio of 18. The inferred masses of the initial black +5:7 +2:8 holes are 30:5 3:0 M and 25:3 4:2 M (at the 90% credible level). The luminosity distance of the source +130 − − +0:03 is 540 210 Mpc, corresponding to a redshift of z =0:11 0:04. A network of three detectors improves the sky localization− of the source, reducing the area of the− 90% credible region from 1160 deg2 using only the two LIGO detectors to 60 deg2 using all three detectors. For the first time, we can test the nature of gravitational wave polarizations from the antenna response of the LIGO-Virgo network, thus enabling a new class of phenomenological tests of gravity. PACS numbers: INTRODUCTION in Virgo and a BBH signal only in the LIGO detectors: the three detector BBH signal model is preferred with a Bayes The era of gravitational wave (GW) astronomy began factor of more than 1600. with the detection of binary black hole (BBH) mergers, Until Advanced Virgo became operational, typical GW by the Advanced Laser Interferometer Gravitational Wave position estimates were highly uncertain compared to the Observatory (LIGO) detectors [1], during the first of the fields of view of most telescopes. -
Polarization Tests of GW170814 and GW170817 Using Waveforms Consistent with Alternative Theories of Gravity
7th KAGRA International Workshop 2020. 12/19 Polarization tests of GW170814 and GW170817 using waveforms consistent with alternative theories of gravity Hiroki Takeda (University of Tokyo), Atsushi Nishizawa, Soichiro Morisaki Polarization Generic metric theory allows 6 polarizations. A = + , × , x, y, b, l Tensor Plus Cross Vector Vector x Plus mode Vector x mode Breathing mode Vector y Scalar Breathing Cross mode Vector y mode Longitudinal mode Longitudinal 2 Tests of GR by polarization Possible polarization modes in a specific theory. Theory Plus Cross Vector x vector y Breathing Longitudinal General Relativity Kaluza-Klein theory Brans-Dicke theory f(R) theory Bimetric theory Separating the polarization modes from detector signals. ->We can test GR by the polarization modes of the gravitational waves. 3 Detector Signal GW amplitude for polarization mode A Detector signal ̂ A ̂ hI(t, Ω) = ∑ FI (Ω)hA A Antenna pattern functions Plus Cross Vector x represent detector response. Vector y Breathing Longitudinal Detector tensor 4 Reconstruction In principle, (The number of polarizations) = (The number of detectors) % × ( ℎ" = $" ℎ% + $" ℎ× + $" ℎ( % × ( e.g. Detector =3, modes = ( + , × , b) ℎ) = $) ℎ% + $) ℎ× + $) ℎ( % × ( ℎ* = $* ℎ% + $* ℎ× + $* ℎ( Reconstruction(Inverse problem) Detector network expansion → More polarizations can be probed. 5 Motivation Bayesian model selection between GR and the theory allowing only scalar or vector by simple substitution of the antenna pattern functions. [LVC(2017)PRL, LVC(2019)PRL.] Tensor vs Vector T V log BTV > 3 (GW170814) hI = FI hT vs hI = FI hT {log BTV = 20.81 (GW170817) Tensor vs Scalar log B > 2.3 (GW170814) T vs S TS hI = FI hT hI = FI hT {log BTS = 23.09 (GW170817) 1.