The Rate of Short-Duration Gamma-Ray Bursts in the Local Universe
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Astronomie in Theorie Und Praxis 8. Auflage in Zwei Bänden Erik Wischnewski
Astronomie in Theorie und Praxis 8. Auflage in zwei Bänden Erik Wischnewski Inhaltsverzeichnis 1 Beobachtungen mit bloßem Auge 37 Motivation 37 Hilfsmittel 38 Drehbare Sternkarte Bücher und Atlanten Kataloge Planetariumssoftware Elektronischer Almanach Sternkarten 39 2 Atmosphäre der Erde 49 Aufbau 49 Atmosphärische Fenster 51 Warum der Himmel blau ist? 52 Extinktion 52 Extinktionsgleichung Photometrie Refraktion 55 Szintillationsrauschen 56 Angaben zur Beobachtung 57 Durchsicht Himmelshelligkeit Luftunruhe Beispiel einer Notiz Taupunkt 59 Solar-terrestrische Beziehungen 60 Klassifizierung der Flares Korrelation zur Fleckenrelativzahl Luftleuchten 62 Polarlichter 63 Nachtleuchtende Wolken 64 Haloerscheinungen 67 Formen Häufigkeit Beobachtung Photographie Grüner Strahl 69 Zodiakallicht 71 Dämmerung 72 Definition Purpurlicht Gegendämmerung Venusgürtel Erdschattenbogen 3 Optische Teleskope 75 Fernrohrtypen 76 Refraktoren Reflektoren Fokus Optische Fehler 82 Farbfehler Kugelgestaltsfehler Bildfeldwölbung Koma Astigmatismus Verzeichnung Bildverzerrungen Helligkeitsinhomogenität Objektive 86 Linsenobjektive Spiegelobjektive Vergütung Optische Qualitätsprüfung RC-Wert RGB-Chromasietest Okulare 97 Zusatzoptiken 100 Barlow-Linse Shapley-Linse Flattener Spezialokulare Spektroskopie Herschel-Prisma Fabry-Pérot-Interferometer Vergrößerung 103 Welche Vergrößerung ist die Beste? Blickfeld 105 Lichtstärke 106 Kontrast Dämmerungszahl Auflösungsvermögen 108 Strehl-Zahl Luftunruhe (Seeing) 112 Tubusseeing Kuppelseeing Gebäudeseeing Montierungen 113 Nachführfehler -
WHAT's BEHIND the MYSTERIOUS GAMMA-RAY BURSTS? LIGO's
WHAT’S BEHIND THE MYSTERIOUS GAMMA-RAY BURSTS? LIGO’s SEARCH FOR CLUES TO THEIR ORIGINS The story of gamma-ray bursts (GRBs) began in the 1960s aboard spacecrafts designed to monitor the former Soviet Union for compliance with the nuclear test ban treaty of 1963. The satellites of the Vela series, each armed with a number of caesium iodide scintillation counters, recorded many puzzling bursts of gamma-ray radiation that did not fit the expected signature of a nuclear weapon. The existence of these bursts became public knowledge in 1973, beginning a decades long quest to understand their origin. Since then, scientists have launched many additional satellites to study these bursts (gamma rays are blocked by the earth's atmosphere) and have uncovered many clues. GRBs occur approximately once a day in a random point in the sky. Most FIGURES FROM THE PUBLICATION GRBs originate millions or billions of light years away. The fact that they For more information on how these figures were generated, and are still so bright by the time they get to earth makes them some of the their meaning, see the publication preprint at arXiv. most energetic astrophysical events observed in the electromagnetic spectrum. In fact, a typical GRB will release in just a handful of seconds as much energy as our sun will throughout its entire life. They can last anywhere from hundredths of seconds to thousands of seconds, but are roughly divided into two categories based on duration (long and short). The line between the two classes is taken to be at 2 seconds (although more sophisticated features are also taken into account in the classification). -
Nanda Rea Institute for Space Science, CSIC-IEEC, Barcelona
Magnetar candidates: new discoveries open new questions Nanda Rea Institute for Space Science, CSIC-IEEC, Barcelona Image Credit: ESA - Christophe Carreau Isolated Neutron Stars: P-Pdot diagram 2 6 4 2 ⎛ 8 2R 6 ⎞ ˙ 2 2 2B R Ω sin α ˙ π ns 2 2 E rot = − m˙˙ = − PP = ⎜ 3 ⎟ B0 sin α 3c 3 3c 3 ⎝ 3c I ⎠ m 2c 3 B = e = 4.414 "1013Gauss Critical Electron Quantum B-field critic e! € Nanda Rea CSIC-IEEC € ! AXPs and SGRs general properties • bright X-ray pulsars Lx ~ 1033-1036 erg/s • strong soft and hard X-ray emission • rotating with periods of ~2-12s and period derivatives of ~10-11-10-13 s/s (Rea et al. 2007) • pulsed fractions ranging from ~5-70 % • magnetic fields of ~1014-1015 Gauss (Rea et al. 2004) (see Mereghetti 2008, A&AR, for a review) Nanda Rea CSIC-IEEC AXPs and SGRs general properties (Kaspi et al. 2003) Short bursts • the most common • they last ~0.1s • peak ~1041 ergs/s • soft γ-rays thermal spectra Intermediate bursts (Israel et al. 2008) • they last 1-40 s • peak ~1041-1043 ergs/s • abrupt on-set • usually soft γ-rays thermal spectra Giant Flares (Palmer et al. 2005) • their output of high energy is exceeded only by blazars and GRBs • peak energy > 3x1044 ergs/s • <1 s initial peak with a hard spectrum which rapidly become softer in the burst tail that can last > 500s, showing the NS spin pulsations. Nanda Rea CSIC-IEEC AXPs and SGRs general properties • transient outbursts lasting months-years • in a few cases radio pulsed emission was observed connected with X-ray outbursts, with variable flux and profiles, and flat spectra (Rea & Esposito 2010, APSS Springer Review) Nanda Rea CSIC-IEEC AXPs and SGRs general properties bursts/outbursts activity !""" &*$..+0$ (6$/&(.$ "-#$/+.)$ #2"$&,/'$ &*$&'(&$ !"" 425$/&//$ 425$&)(,$ !" 425$&,&($ "-#$&'/)$ "-#$/+/&$ "-#$&0//$ "-#$&'11$ &*$&/('$ ! '()*+,- 23*$&'&/$ "#! "-#$&).,$ !"#$%&'()$ !"#$&)..$ "#"! &*$&+(,$ !"ï& "#$! % $ !" %" ./0!"!1/23 Nanda Rea CSIC-IEEC Why magnetars behave differently from normal pulsars? • Their internal magnetic field is twisted up to 10 times the external dipole. -
Massive Fast Rotating Highly Magnetized White Dwarfs: Theory and Astrophysical Applications
Massive Fast Rotating Highly Magnetized White Dwarfs: Theory and Astrophysical Applications Thesis Advisors Ph.D. Student Prof. Remo Ruffini Diego Leonardo Caceres Uribe* Dr. Jorge A. Rueda *D.L.C.U. acknowledges the financial support by the International Relativistic Astrophysics (IRAP) Ph.D. program. Academic Year 2016–2017 2 Contents General introduction 4 1 Anomalous X-ray pulsars and Soft Gamma-ray repeaters: A new class of pulsars 9 2 Structure and Stability of non-magnetic White Dwarfs 21 2.1 Introduction . 21 2.2 Structure and Stability of non-rotating non-magnetic white dwarfs 23 2.2.1 Inverse b-decay . 29 2.2.2 General Relativity instability . 31 2.2.3 Mass-radius and mass-central density relations . 32 2.3 Uniformly rotating white dwarfs . 37 2.3.1 The Mass-shedding limit . 38 2.3.2 Secular Instability in rotating and general relativistic con- figurations . 38 2.3.3 Pycnonuclear Reactions . 39 2.3.4 Mass-radius and mass-central density relations . 41 3 Magnetic white dwarfs: Stability and observations 47 3.1 Introduction . 47 3.2 Observations of magnetic white dwarfs . 49 3.2.1 Introduction . 49 3.2.2 Historical background . 51 3.2.3 Mass distribution of magnetic white dwarfs . 53 3.2.4 Spin periods of isolated magnetic white dwarfs . 53 3.2.5 The origin of the magnetic field . 55 3.2.6 Applications . 56 3.2.7 Conclusions . 57 3.3 Stability of Magnetic White Dwarfs . 59 3.3.1 Introduction . 59 3.3.2 Ultra-magnetic white dwarfs . 60 3.3.3 Equation of state and virial theorem violation . -
Gamma Ray Bursts, Their Afterglows, and Soft Gamma Repeaters
Gamma ray bursts, their afterglows, . and soft gamma repeaters G.S.Bisnovatyi-Kogan IKI RAS, Moscow GRB Workshop 2012 Moscow University June 14 Estimations Central GRB machne Afterglow SGR Nuclear model of SGR Neutron stars are the result of collapse . Conservation of the magnetic flux 2 B(ns)=B(s) (Rs /Rns ) B(s)=10 – 100 Gs, R ~ (3 – 10) R( Sun ), R =10 km s ns B(ns) = 4 10 11– 5 10 13 Gs Ginzburg (1964) Radiopulsars E = AB2 Ω 4 - magnetic dipole radiation (pulsar wind) 2 E = 0.5 I Ω I – moment of inertia of the neutron star 2 B = IPP/4 π A Single radiopulsars – timing observations (the most rapid ones are connected with young supernovae remnants) 11 13 B(ns) = 2 10 – 5 10 Gs Neutron star formation N.V.Ardeljan, G.S.Bisnovatyi-Kogan, S.G.Moiseenko MNRAS, 4E+51 Ekinpol 2005, 359 , 333 . E 3.5E+51 rot Emagpol Emagtor 3E+51 2.5E+51 2E+51 B(chaotic) ~ 10^14 Gs 1.5E+51 1E+51 High residual chaotic 5E+50 magnetic field after MRE core collapse SN explosion. 0 0.1 0.2 0.3 0.4 0.5 Heat production during time,sec Ohmic damping of the chaotic magnetic field may influence NS cooling light curve Inner region: development of magnetorotational instability (MRI) TIME= 34.83616590 ( 1.20326837sec ) TIME= 35.08302173 ( 1.21179496sec ) 0 .0 1 4 0 .0 1 4 0 .0 1 3 0 .0 1 3 0 .0 1 2 0 .0 1 2 0 .0 1 1 0 .0 1 1 0 .0 1 0 .0 1 0 .0 0 9 0 .0 0 9 Z 0 .0 0 8 0Z .0 0 8 0 .0 0 7 0 .0 0 7 0 .0 0 6 0 .0 0 6 0 .0 0 5 0 .0 0 5 0 .0 0 4 0 .0 0 4 0 .0 0 3 0 .0 0 3 0 .0 0 2 0 .0 0 2 0 .0 1 0 .0 1 5 0 .0 2 0 .0 1 0 .0 1 5 0 .0 2 R R TIME= 35.26651529 ( 1.21813298sec ) TIME= -
Mission Design Concept
AXTAR: mission design concept Paul S. Raya, Deepto Chakrabartyb, Colleen A. Wilson-Hodgec, Bernard F. Phlipsa, Ronald A. Remillardb, Alan M. Levineb, Kent S. Wooda, Michael T. Wolffa, Chul S. Gwona, Tod E. Strohmayerd, Michael Baysingere, Michael S. Briggsc, Peter Capizzoe, Leo Fabisinskie, Randall C. Hopkinse, Linda S. Hornsbye, Les Johnsone, C. Dauphne Maplese, Janie H. Miernike, Dan Thomase, Gianluigi De Geronimof aSpace Science Division, Naval Research Laboratory, Washington, DC 20375, USA bKavli Institute for Astrophysics and Space Research, Massachusetts Institute of Technology, Cambridge, MA 02139, USA cSpace Science Office, NASA Marshall Space Flight Center, Huntsville, AL 35812, USA dNASA Goddard Space Flight Center, Greenbelt, MD 20771, USA eAdvanced Concepts Office, NASA Marshall Space Flight Center, Huntsville, AL 35812, USA fInstrumentation Division, Brookhaven National Laboratory, Upton, NY 11973, USA ABSTRACT The Advanced X-ray Timing Array (AXTAR) is a mission concept for X-ray timing of compact objects that combines very large collecting area, broadband spectral coverage, high time resolution, highly flexible scheduling, and an ability to respond promptly to time-critical targets of opportunity. It is optimized for submillisecond timing of bright Galactic X-ray sources in order to study phenomena at the natural time scales of neutron star surfaces and black hole event horizons, thus probing the physics of ultradense matter, strongly curved spacetimes, and intense magnetic fields. AXTAR’s main instrument, the Large Area Timing Array (LATA) is a collimated instrument with 2–50 keV coverage and over 3 square meters effective area. The LATA is made up of an array of supermodules that house 2-mm thick silicon pixel detectors. -
No Supernovae Associated with Two Long-Duration Γ-Ray Bursts
1 No supernovae associated with two long-duration γ-ray bursts Johan P. U. Fynbo1, Darach Watson1, Christina C. Thöne1, Jesper Sollerman1,2, Joshua S. Bloom3, Tamara M. Davis1, Jens Hjorth1, Páll Jakobsson4, Uffe G. Jørgensen5, John F. Graham6, Andrew S. Fruchter6, David Bersier7, Lisa Kewley8, Arnaud Cassan9, José María Castro Cerón1, Suzanne Foley10, Javier Gorosabel11, Tobias C. Hinse5, Keith D. Horne12, Brian L. Jensen1, Sylvio Klose13, Daniel Kocevski3, Jean-Baptiste Marquette14, Daniel Perley3, Enrico Ramirez-Ruiz15,16, Maximilian D. Stritzinger1, Paul M. Vreeswijk17,18, Ralph A. M. Wijers19, Kristian G. Woller5, Dong Xu1, Marta Zub6 1Dark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen, Denmark 2Department of Astronomy, Stockholm University, Sweden 3Department of Astronomy, University of California at Berkeley, 601 Campbell Hall, Berkeley, CA 94720, USA 4Centre for Astrophysics Research, University of Hertfordshire, College Lane, Hatfield, Herts, AL10 9AB, UK 5Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen, Denmark 6Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, Maryland 21218, USA 7Astrophysics Research Institute, Liverpool John Moores University, Twelve Quays House, Egerton Wharf, Birkenhead CH41 1LD, UK 2 8University of Hawaii, Institute of Astronomy, 2680 Woodlawn Drive, Honolulu, HI 96822, US 9Astronomisches Rechen-Institut (ARI), Zentrum für Astronomie der Universität Heidelberg (ZAH), Mönchof Str. -
Cviewoftherestlesssn2009ip Reveals the Explosive Ejection of a Massive Star Envelope Margutti, R., Et Al
1 Peter J. Brown Office Address Contact Information M311 Mitchell Institute for Fundamental Physics and Astronomy E-mail: [email protected] Department of Physics & Astronomy, Texas A&M University Cell: (979) 402-4523 Skype: grbpeter 4242 TAMU, College Station, TX 77843 www.linkedin.com/in/peter-brown-supernova Highlights Observational Astrophysicist with experience in ground and space-based Ultraviolet and• Optical Photometry and Spectroscopy of Supernovae and other Transients Leader of Swift supernova team since 2005 and Swift Cycle 14 Key Project • PI of 5 Hubble Space Telescope Programs • Principal Investigator of External Grants Totaling over $2,600,000 • 18 Refereed, First Author Journal Articles, 140+ Coauthored Journal Articles • 2017 Texas A&M College of Science Undergraduate Research Mentoring Award • Education Ph.D. in Astronomy & Astrophysics – Pennsylvania State University August 2009 Thesis Title: “The Ultraviolet Properties of Supernovae” Thesis Advisor: Dr. P. W. A. Roming B.S. in Physics and Astronomy – Brigham Young University August 2004 Senior Thesis Title: “Observing Gamma Ray Burst Afterglows from BYU’s Orson Pratt Observatory” Thesis Advisor: Professor J. W. Moody Academic Research Scientist – Mitchell Institute, Texas A&M University 2016 – present Positions Visiting Associate Professor Spring 2020 Visiting Assistant Professor Spring 2018 Mitchell Fellow, Postdoctoral Research Associate 2012 – 2016 Supervisor: Professor Lifan Wang Postdoctoral Research Associate – University of Utah 2009 – 2012 Supervisor: Professor -
Liverpool Telescope 2: a New Robotic Facility for Rapid Transient Follow-Up
Noname manuscript No. (will be inserted by the editor) Liverpool Telescope 2: a new robotic facility for rapid transient follow-up C.M. Copperwheat · I.A. Steele · R.M. Barnsley · S.D. Bates · D. Bersier · M.F. Bode · D. Carter · N.R. Clay · C.A. Collins · M.J. Darnley · C.J. Davis · C.M. Gutierrez · D.J. Harman · P.A. James · J.H. Knapen · S. Kobayashi · J.M. Marchant · P.A. Mazzali · C.J. Mottram · C.G. Mundell · A. Newsam · A. Oscoz · E. Palle · A. Piascik · R. Rebolo · R.J. Smith Received: date / Accepted: date Abstract The Liverpool Telescope is one of the world’s premier facilities for time domain astronomy. The time domain landscape is set to radically change in the coming decade, with synoptic all-sky surveys such as LSST providing huge numbers of transient detections on a nightly basis; transient detections across the electromagnetic spectrum from other major facilities such as SVOM, SKA and CTA; and the era of ‘multi-messenger astronomy’, wherein astro- physical events are detected via non-electromagnetic means, such as neutrino or gravitational wave emission. We describe here our plans for the Liverpool Telescope 2: a new robotic telescope designed to capitalise on this new era of time domain astronomy. LT2 will be a 4-metre class facility co-located with the Liverpool Telescope at the Observatorio del Roque de Los Muchachos on the Canary island of La Palma. The telescope will be designed for extremely C.M. Copperwheat · I.A. Steele · R.M. Barnsley · S.D. Bates · D. Bersier · M.F. Bode · D. -
Short Burst GRB 060614
ARTICLE Received 8 Oct 2014 | Accepted 27 Apr 2015 | Published 11 Jun 2015 DOI: 10.1038/ncomms8323 OPEN A possible macronova in the late afterglow of the long–short burst GRB 060614 Bin Yang1,2, Zhi-Ping Jin1, Xiang Li1,2, Stefano Covino3, Xian-Zhong Zheng1, Kenta Hotokezaka4, Yi-Zhong Fan1,5, Tsvi Piran4 & Da-Ming Wei1 Long-duration (42s) g-ray bursts that are believed to originate from the death of massive stars are expected to be accompanied by supernovae. GRB 060614, that lasted 102 s, lacks a supernova-like emission down to very stringent limits and its physical origin is still debated. Here we report the discovery of near-infrared bump that is significantly above the regular decaying afterglow. This red bump is inconsistent with even the weakest known supernova. However, it can arise from a Li-Paczyn´ski macronova—the radioactive decay of debris following a compact binary merger. If this interpretation is correct, GRB 060614 arose from a compact binary merger rather than from the death of a massive star and it was a site of a significant production of heavy r-process elements. The significant ejected mass favours a black hole–neutron star merger but a double neutron star merger cannot be ruled out. 1 Key Laboratory of Dark Matter and Space Astronomy, Purple Mountain Observatory, Chinese Academy of Sciences, Nanjing 210008, China. 2 University of Chinese Academy of Sciences, Yuquan Road 19, Beijing 100049, China. 3 INAF/Brera Astronomical Observatory, via Bianchi 46, I-23807 Merate, Italy. 4 Racah Institute of Physics, The Hebrew University, Jerusalem 91904, Israel. -
Noao Annual Report Fy07
AURA/NOAO ANNUAL REPORT FY 2007 Submitted to the National Science Foundation September 30, 2007 Revised as Final and Submitted January 30, 2008 Emission nebula NGC6334 (Cat’s Paw Nebula): star-forming region in the constellation Scorpius. This 2007 image was taken using the Mosaic-2 imager on the Blanco 4-meter telescope at Cerro Tololo Inter- American Observatory. Intervening dust in the plane of the Milky Way galaxy reddens the colors of the nebula. Image credit: T.A. Rector/University of Alaska Anchorage, T. Abbott and NOAO/AURA/NSF NATIONAL OPTICAL ASTRONOMY OBSERVATORY NOAO ANNUAL REPORT FY 2007 Submitted to the National Science Foundation September 30, 2007 Revised as Final and Submitted January 30, 2008 TABLE OF CONTENTS EXECUTIVE SUMMARY ............................................................................................................................. 1 1 SCIENTIFIC ACTIVITIES AND FINDINGS ..................................................................................... 2 1.1 NOAO Gemini Science Center .............................................................................. 2 GNIRS Infrared Spectroscopy and the Origins of the Peculiar Hydrogen-Deficient Stars...................... 2 Supermassive Black Hole Growth and Chemical Enrichment in the Early Universe.............................. 4 1.2 Cerro Tololo Inter-American Observatory (CTIO)................................................ 5 The Nearest Stars....................................................................................................................................... -
Tev Gamma Rays from Galactic Center Pulsars
FERMILAB-PUB-17-173-A (accepted) DOI:10.1016/j.dark.2018.05.004 FERMILAB-PUB-17-173-A Prepared for submission to JCAP TeV Gamma Rays From Galactic Center Pulsars Dan Hooper,a;b;c Ilias Cholisd and Tim Lindene aFermi National Accelerator Laboratory, Center for Particle Astrophysics, Batavia, IL 60510 bUniversity of Chicago, Department of Astronomy and Astrophysics, Chicago, IL 60637 cUniversity of Chicago, Kavli Institute for Cosmological Physics, Chicago, IL 60637 dDepartment of Physics and Astronomy, The Johns Hopkins University, Baltimore, Mary- land, 21218 eOhio State University, Center for Cosmology and AstroParticle Physics (CCAPP), Colum- bus, OH 43210 E-mail: [email protected], [email protected], [email protected] Abstract. Measurements of the nearby pulsars Geminga and B0656+14 by the HAWC and Milagro telescopes have revealed the presence of bright TeV-emitting halos surrounding these objects. If young and middle-aged pulsars near the Galactic Center transfer a similar fraction of their energy into TeV photons, then these sources could plausibly dominate the emission that is observed by HESS and other ground-based telescopes from the innermost 102 parsecs of the Milky Way. In particular, both the spectral shape and the angular extent∼ of this emission is consistent with TeV halos produced by a population of pulsars, although the reported correlation of this emission with the distribution of molecular gas suggests that diffuse hadronic processes also must contribute. The overall flux of this emission requires a birth rate of 100-1000