Gamma-Ray Burst Afterglows: Surprises from The
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
The Optical Afterglow of GRB 000911: Evidence for an Associated Supernova??
A&A 378, 996–1002 (2001) Astronomy DOI: 10.1051/0004-6361:20011282 & c ESO 2001 Astrophysics The optical afterglow of GRB 000911: Evidence for an associated supernova?? D. Lazzati1,S.Covino2, G. Ghisellini2,D.Fugazza2,S.Campana2,P.Saracco2,P.A.Price3,4,E.Berger3, S. Kulkarni3, E. Ramirez–Ruiz1,A.Cimatti5, M. Della Valle5, S. di Serego Alighieri5,A.Celotti6, F. Haardt7,G.L.Israel8, and L. Stella8 1 Institute of Astronomy, University of Cambridge, Madingley Road, CB3 0HA Cambridge, UK 2 Osservatorio Astronomico di Brera, Via Bianchi 46, 23807 Merate (Lc), Italy 3 Palomar Observatory, 105-24, California Institute of Technology, Pasadena, CA 91125, USA 4 Research School of Astronomy & Astrophysics, Mount Stromlo Observatory, Cotter Road, Weston, ACT 2611, Australia 5 Osservatorio Astrofisico di Arcetri, Largo E. Fermi 5, 50125 Firenze, Italy 6 SISSA/ISAS, via Beirut 4, 34014 Trieste, Italy 7 Universit`a dell’Insubria, Via Lucini 3, 22100 Como, Italy 8 Osservatorio Astronomico di Roma, Via Frascati 33, 00040 Monteporzio Catone, Italy Received 12 July 2001 / Accepted 12 September 2001 Abstract. We present photometric and spectroscopic observations of the late afterglow of GRB 000911, starting ∼1 day after the burst event and lasting ∼8 weeks. We detect a moderately significant re–brightening in the R, I and J lightcurves, associated with a sizable reddening of the spectrum. This can be explained through the presence of an underlying supernova, outshining the afterglow ∼30 days after the burst event. Alternative explanations are discussed. Key words. gamma rays: bursts – supernovae: general 1. Introduction (Djorgovskij et al. 1999), a moderate amount of multiband data but lacked spectroscopic coverge. -
Arxiv:0809.0508V2 [Astro-Ph]
Accepted in ApJ on Nov 13 2008 Preprint typeset using LATEX style emulateapj v. 08/22/09 THE PROPERTIES OF THE HOST GALAXY AND THE IMMEDIATE ENVIRONMENT OF GRB 980425 / SN 1998BW FROM THE MULTI-WAVELENGTH SPECTRAL ENERGY DISTRIBUTION Micha lJ. Micha lowski1, Jens Hjorth1, Daniele Malesani1, Tadeusz Micha lowski2, Jose´ Mar´ıa Castro Ceron´ 1, Robert F. Reinfrank3,4, Michael A. Garrett5,6,7, Johan P. U. Fynbo1, Darach J. Watson1 and Uffe G. Jørgensen8 Accepted in ApJ on Nov 13 2008 ABSTRACT We present an analysis of the spectral energy distribution (SED) of the galaxy ESO 184-G82, the host of the closest known long gamma-ray burst (GRB) 980425 and its associated supernova (SN) 1998bw. We use our observations obtained at the Australia Telescope Compact Array (the third > 3σ radio detection of a GRB host) as well as archival infrared and ultraviolet (UV) observations to estimate its star formation state. We find that ESO 184-G82 has a UV star formation rate (SFR) and stellar mass consistent with the population of cosmological GRB hosts and of local dwarf galaxies. However, it has a higher specific SFR (per unit stellar mass) than luminous spiral galaxies. The mass of ESO 184-G82 is dominated by an older stellar population in contrast to the majority of GRB hosts. The Wolf-Rayet region ∼ 800 pc from the SN site experienced a starburst episode during which the majority of its stellar population was built up. Unlike that of the entire galaxy, its SED is similar to those of cosmological submillimeter/radio-bright GRB hosts with hot dust content. -
On the Association of Gamma-Ray Bursts with Supernovae Dieter H
Clemson University TigerPrints Publications Physics and Astronomy Summer 7-24-1998 On the Association of Gamma-Ray Bursts with Supernovae Dieter H. Hartmann Department of Physics and Astronomy, Clemson University, [email protected] R. M. Kippen Center for Space Plasma and Aeronomic Research, University of Alabama in Huntsville & NASA/Marshall Space Flight Center & NASA/Marshall Space Flight Center M. S. Briggs Physics Department, University of Alabama in Huntsville & NASA/Marshall Space Flight Center J. M. Kommers Department of Physics and Center for Space Research, Massachusetts nI stitute of Technology C. Kouveliotou Universities Space Research Association & NASA/Marshall Space Flight Center See next page for additional authors Follow this and additional works at: https://tigerprints.clemson.edu/physastro_pubs Recommended Citation Please use publisher's recommended citation. This Article is brought to you for free and open access by the Physics and Astronomy at TigerPrints. It has been accepted for inclusion in Publications by an authorized administrator of TigerPrints. For more information, please contact [email protected]. Authors Dieter H. Hartmann, R. M. Kippen, M. S. Briggs, J. M. Kommers, C. Kouveliotou, K. Hurley, C. R. Robinson, J. van Paradijs, T. J. Galama, and P. M. Vresswijk This article is available at TigerPrints: https://tigerprints.clemson.edu/physastro_pubs/83 Re-Submitted to ApJL 24-Jul-98 On the Association of Gamma-Ray Bursts with Supernovae R. M. Kippen,1,2,3 M. S. Briggs,4,2 J. M. Kommers,5 C. Kouveliotou,6,2 K. Hurley,7 C. R. Robinson,6,2 J. van Paradijs,5,8 D. H. Hartmann,9 T. -
Physical Parameters of GRB 970508 and GRB 971214 from Their
SUBMITTED 22-APR-99 TO ASTROPHYSICAL JOURNAL, IN ORIGNAL FORM 26-MAY-98 Preprint typeset using LATEX style emulateapj PHYSICAL PARAMETERS OF GRB 970508 AND GRB 971214 FROM THEIR AFTERGLOW SYNCHROTRON EMISSION R.A.M.J. WIJERS1 AND T.J. GALAMA2 SUBMITTED 22-APR-99 to Astrophysical Journal, in orignal form 26-MAY-98 ABSTRACT We have calculated synchrotron spectra of relativistic blast waves, and find predicted characteristic frequencies that are more than an order of magnitude different from previous calculations. For the case of an adiabatically expanding blast wave, which is applicable to observed gamma-ray burst (GRB) afterglows at late times, we give expressions to infer the physical properties of the afterglow from the measured spectral features. We show that enough data exist for GRB970508to compute unambiguously the ambient density, n =0.03cm−3, and the blast wave energy per unit solid angle, =3 1052 erg/4π sr. We also compute the energy density in electrons and magnetic field. We find that they areE 12%× and 9%, respectively, of the nucleon energy density and thus confirm for the first time that both are close to but below equipartition. For GRB971214,we discuss the break found in its spectrum by Ramaprakash et al. (1998). It can be interpreted either as the peak frequency or as the cooling frequency; both interpretations have some problems, but on balance the break is more likely to be the cooling frequency. Even when we assume this, our ignorance of the self- absorption frequency and presence or absence of beaming make it impossible to constrain the physical parameters of GRB971214 very well. -
An Apparently Normal G-Ray Burst with an Unusually Low Luminosity
letters to nature .............................................................. energy equivalent over the 20–2000 keV band, we find 6 £ 49 50 10 erg , e g,iso , 1.4 £ 10 erg; where the range reflects the An apparently normal g-ray burst observational uncertainty in the spectrum above 200 keV (see with an unusually low luminosity Fig. 2). GRB 031203, an event with spectrum similar to cosmological S. Yu. Sazonov1,2, A. A. Lutovinov1 & R. A. Sunyaev1,2 GRBs, is the least energetic (in terms of e g,iso) long-duration GRB. Clearly, g-ray luminosities and energy releases vary widely, span- 1Space Research Institute, Russian Academy of Sciences, Profsoyuznaya 84/32, ning at least four orders of magnitude. Furthermore it is of 117997 Moscow, Russia considerable interest to note that GRB 031203 violates two much 2 Max-Planck-Institut fu¨r Astrophysik, Karl-Schwarzschild-Str. 1, D-85740 discussed relations in GRB astrophysics: (1) the e g,iso–E peak relation Garching bei Mu¨nchen, Germany and (2) the luminosity–spectral lag relation. For GRB 031203, the ............................................................................................................................................................................. 4 first relation predicts E peak < 10 keV, in gross disagreement with Much of the progress in understanding g-ray bursts (GRBs) has the analysis presented here. Long spectral lags are expected from the come from studies of distant events (redshift z < 1). In the second relation5,6 when in fact we see virtually no lag (Fig. 3). brightest GRBs, the g-rays are so highly collimated that the GRB 031203, however, shares some properties with GRB 980425, events can be seen across the Universe. It has long been suspected which is associated with a nearby (z ¼ 0.0085) supernova, SN that the nearest and most common events have been missed 1998bw (refs 14, 15). -
Evidence for Supernova Light in All Gamma-Ray Burst Afterglow A
Clemson University TigerPrints Publications Physics and Astronomy Winter 12-13-2004 Evidence for Supernova Light in all Gamma-Ray Burst Afterglow A. Zeh Thüringer Landessternwarte Tautenburg S. Klose Thüringer Landessternwarte Tautenburg Dieter H. Hartmann Department of Physics and Astronomy, Clemson University, [email protected] Follow this and additional works at: https://tigerprints.clemson.edu/physastro_pubs Recommended Citation Please use publisher's recommended citation. This Article is brought to you for free and open access by the Physics and Astronomy at TigerPrints. It has been accepted for inclusion in Publications by an authorized administrator of TigerPrints. For more information, please contact [email protected]. 22nd Texas Symposium on Relativistic Astrophysics at Stanford University, Dec. 13-17, 2004 Evidence for Supernova Light in All Gamma-Ray Burst Afterglows A. Zeh, S. Klose Thur¨ inger Landessternwarte Tautenburg, 07778 Tautenburg, Germany D. H. Hartmann Department of Physics and Astronomy, Clemson University, Clemson, SC 29634-0978 We present an update of our systematic analyses of all Gamma-Ray Burst (GRB) afterglow data, now published through the end of 2004, in an attempt to detect the predicted supernova light component. We fit the observed photometric light curves as the sum of an afterglow, an underlying host galaxy, and a supernova component. The latter is modeled using published UBV RI light curves of SN 1998bw as a template. The total sample of afterglows with established redshifts contains now 29 bursts (GRB 970228 - GRB 041006). For 13 of them a weak supernova excess (scaled to SN 1998bw) was found. In agreement with our earlier result [47] we find that also in the updated sample all bursts with redshift ∼< 0.7 show a supernova excess in their afterglow light curves. -
Gravitational Waves and Gamma-Rays from a Binary Neutron Star Merger: Gw170817 and Grb 170817A
Draft version October 15, 2017 Typeset using LATEX twocolumn style in AASTeX61 GRAVITATIONAL WAVES AND GAMMA-RAYS FROM A BINARY NEUTRON STAR MERGER: GW170817 AND GRB 170817A B. P. Abbott,1 R. Abbott,1 T. D. Abbott,2 F. Acernese,3, 4 K. Ackley,5, 6 C. Adams,7 T. Adams,8 P. Addesso,9 R. X. Adhikari,1 V. B. Adya,10 C. Affeldt,10 M. Afrough,11 B. Agarwal,12 M. Agathos,13 K. Agatsuma,14 N. Aggarwal,15 O. D. Aguiar,16 L. Aiello,17, 18 A. Ain,19 P. Ajith,20 B. Allen,10, 21, 22 G. Allen,12 A. Allocca,23, 24 M. A. Aloy,25 P. A. Altin,26 A. Amato,27 A. Ananyeva,1 S. B. Anderson,1 W. G. Anderson,21 S. V. Angelova,28 S. Antier,29 S. Appert,1 K. Arai,1 M. C. Araya,1 J. S. Areeda,30 N. Arnaud,29, 31 K. G. Arun,32 S. Ascenzi,33, 34 G. Ashton,10 M. Ast,35 S. M. Aston,7 P. Astone,36 D. V. Atallah,37 P. Aufmuth,22 C. Aulbert,10 K. AultONeal,38 C. Austin,2 A. Avila-Alvarez,30 S. Babak,39 P. Bacon,40 M. K. M. Bader,14 S. Bae,41 P. T. Baker,42 F. Baldaccini,43, 44 G. Ballardin,31 S. W. Ballmer,45 S. Banagiri,46 J. C. Barayoga,1 S. E. Barclay,47 B. C. Barish,1 D. Barker,48 K. Barkett,49 F. Barone,3, 4 B. Barr,47 L. Barsotti,15 M. Barsuglia,40 D. Barta,50 J. -
L105 EXPECTED CHARACTERISTICS of the SUBCLASS of SUPERNOVA GAMMA-RAY BURSTS J. S. BLOOM,1 S. R. Kulkarni, F. HARRISON, T. PRINCE
The Astrophysical Journal, 506:L105±L108, 1998 October 20 q 1998. The American Astronomical Society. All rights reserved. Printed in U.S.A. EXPECTED CHARACTERISTICS OF THE SUBCLASS OF SUPERNOVA GAMMA-RAY BURSTS J. S. Bloom,1 S. R. Kulkarni, F. Harrison, T. Prince, and E. S. Phinney Division of Physics, Mathematics, and Astronomy, California Institute of Technology, Pasadena, CA 91125 and D. A. Frail National Radio Astronomy Observatory, P.O. Box 0, Socorro, NM 87801 Received 1998 July 8; accepted 1998 August 18; published 1998 September 10 ABSTRACT The spatial and temporal coincidence of gamma-ray burst (GRB) 980425 and supernova (SN) 1998bw has prompted speculation that there exists a subclass of GRBs produced by SNe (ªS-GRBsº). A physical model motivated by radio observations lead us to propose the following characteristics of S-GRBs: (1) prompt radio emission and an implied high brightness temperature close to the inverse Compton limit, (2) high expansion velocity (*50,000 km s21) of the optical photosphere as derived from lines widths and energy release larger than usual, (3) no long-lived X-ray afterglow, and (4) a single-pulse GRB pro®le. Radio studies of previous SNe show that only (but not all) Type Ib and Ic SNe potentially satisfy the ®rst condition. We investigate the proposed associations of GRBs and SNe within the context of these proposed criteria and suggest that 1% of GRBs detected by BATSE may be members of this subclass. » Subject headings: gamma rays: bursts Ð supernovae: general Ð supernovae: individual (SN 1998bw) 1. INTRODUCTION common are S-GRBs? How can they be distinguished from C-GRBs? What are their typical energetics? With the spectroscopic observations of the optical afterglow In this paper, accepting the physical model advocated by of gamma-ray burst (GRB) 970508 by Metzger et al. -
Explosive Nucleosynthesis in GRB Jets Accompanied by Hypernovae
SLAC-PUB-12126 astro-ph/0601111 September 2006 Explosive Nucleosynthesis in GRB Jets Accompanied by Hypernovae Shigehiro Nagataki1,2, Akira Mizuta3, Katsuhiko Sato4,5 ABSTRACT Two-dimensional hydrodynamic simulations are performed to investigate ex- plosive nucleosynthesis in a collapsar using the model of MacFadyen and Woosley (1999). It is shown that 56Ni is not produced in the jet of the collapsar suffi- ciently to explain the observed amount of a hypernova when the duration of the explosion is ∼10 sec, which is considered to be the typical timescale of explosion in the collapsar model. Even though a considerable amount of 56Ni is synthesized if all explosion energy is deposited initially, the opening angles of the jets become too wide to realize highly relativistic outflows and gamma-ray bursts in such a case. From these results, it is concluded that the origin of 56Ni in hypernovae associated with GRBs is not the explosive nucleosynthesis in the jet. We consider that the idea that the origin is the explosive nucleosynthesis in the accretion disk is more promising. We also show that the explosion becomes bi-polar naturally due to the effect of the deformed progenitor. This fact suggests that the 56Ni synthesized in the accretion disk and conveyed as outflows are blown along to the rotation axis, which will explain the line features of SN 1998bw and double peaked line features of SN 2003jd. Some fraction of the gamma-ray lines from 56Ni decays in the jet will appear without losing their energies because the jet becomes optically thin before a considerable amount of 56Ni decays as long as the jet is a relativistic flow, which may be observed as relativistically Lorentz boosted line profiles in future. -
Expected Characteristics of the Subclass of Supernova Gamma-Ray Bursts (S-Grbs)
CORE Metadata, citation and similar papers at core.ac.uk Provided by CERN Document Server Expected characteristics of the subclass of Supernova Gamma-ray Bursts (S-GRBs) J. S. Bloom1, S. R. Kulkarni, F. Harrison, T. Prince, E. S. Phinney California Institute of Technology, MS 105-24, Pasadena, CA 91125 and D. A. Frail National Radio Astronomy Observatory, P. O. Box 0, Socorro, NM 87801 ABSTRACT The spatial and temporal coincidence between the gamma-ray burst (GRB) 980425 and supernova (SN) 1998bw has prompted speculation that there exists a class of GRBs produced by SNe (“S-GRBs”). Robust arguments for the existence of a relativistic shock have been presented on the basis of radio observations. A physical model based on the radio observations lead us to propose the following characteristics of supernovae GRBs (S-GRBs): 1) prompt radio emission and implied brightness temperature near or below the inverse Compton limit, 2) high expansion velocity (∼> 50, 000 km/s) of the optical photosphere as derived from lines widths and energy release larger than usual, 3) no long-lived X-ray afterglow, and 4) a single pulse (SP) GRB profile. Radio studies of previous SNe show that only type Ib and Ic potentially satisfy the first condition. Accordingly we have investigated proposed associations of GRBs and SNe finding no convincing evidence (mainly to paucity of data) to confirm any single connection of a SN with a GRB. If there is a more constraining physical basis for the burst time-history of S-GRBs beyond that of the SP requirement, we suggest the 1% of light curves in the BATSE catalogue similar to that of GRB 980425 may constitute the subclass. -
1 the X-Ray Telescope on Board Swift
1 THE X-RAY TELESCOPE ON BOARD SWIFT: STATUS AND MAIN RESULTS G. Tagliaferri1, S. Campana1, G. Chincarini1,2, P. Giommi3, G. Cusumano4, D.N. Burrows5, J.E. Hill5,6, J.A. Kennea5, J.A. Nousek5, J.P. Osborne7, P.T. O’Brien7, A. Wells7, L. Angelini6, and on behalf of the XRT team1 1INAF-Osservatorio Astronomico di Brera, Via Bianchi 46, 23807 Merate, Italy 2Universita` degli Studi di Milano-Bicocca, P.za delle Scienze 3, 20126 Milano, Italy 3ASI Science Data Center, Via G. Galilei, 00044 Frascati, Italy 4INAF-IASF Palermo, Via U. La Malfa 153, 90146 Palermo, Italy 5Pennsylvania State University, 525 Davey Lab, University Park, PA 16802, USA 6NASA Goddard Space Flight Center, MD 20771, USA 7University of Leicester, Department of Physics and Astronomy, Leicester, LE 17 RH, UK ABSTRACT of the GRBs, if not all, had an associated X-ray after- glow only about 60% of them had also an optical after- glow, i.e. a good fraction of them were dark–GRBs. For The X-ray Telescope (XRT), on board the Swift satellite, a general review on these topics see Zhang & Meszaros provides: automated source detection and position with (2004) and Piran (2005). Therefore, it was clear that to few arcsecond accuracy within few seconds from target properly study the GRBs, and in particular the associ- acquisition; CCD spectroscopy and imaging capability ated afterglows, we needed a fast-reaction satellite capa- (0.2-10 keV), with the capability of detecting a milliCrab ble of detecting GRBs and of performing immediate mul- source in about 10 seconds; automatic adjusting of the tiwavelength follow-up observations, in particular in the CCD readout mode to optimize the science return as the X-ray and optical bands. -
Lecture 19 Black Holes and Gamma-Ray Bursts
Black holes in nature – end points of stellar evolution • In our galaxy alone, theory suggests 50 million black holes (2 SN per century for 1010 years ¼ of which make black holes • Most massive galaxies have massive black holes Lecture 19 at their centers (109 galaxies) • Dozens of black hole binary x-ray sources per Black Holes and galaxy – at least Gamma-Ray Bursts • One gravitational radiation detection so far http://apod.nasa.gov/apod/astropix.html They are out there… Some Properties of Black Holes Kinds of black holes: • Entirely defined by their mass, rotation rate, and charge. All memory of how the hole was made Mass Size is lost. Almost like an elementary particle. “Black holes Class have no hair” (Wheeler, Israel, Hawking, etc.) (solar masses) • Believed that all the mass is concentrated at the AGN Supermassive ~105 - 1010 0.001 - 10 AU center in a small quantum-mechanical singularity Intermediate ~1000 ~ R • The effective density of stellar mass black holes, as ? earth defined by their event horizons is very high, but there are supermassive black hole in active galactic nuclei Stellar ~10 ~30 km with average densities no greater than water. they are just XRBin very big (this ignores the central concentration in a singularity though.) The average density matters to tidal forces. ? Primordial Up to ~Moon Up to ~0.1 mm • The gravitational field of a black hole close to the event horizon is complicated, but by the time you are ⎛ 2GM ⎞ ⎛ M ⎞ RS = 2 = 2.96 km ⎜ ⎟ several Schwarzschild radii away, it is indistinguishable ⎜ c ⎟ M ⎝ ⎠ ⎝ ⎠ from that of an ordinary star.