On the Consistency of Peculiar Grbs 060218 and 060614 with the $E
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JOHN R. THORSTENSEN Address
CURRICULUM VITAE: JOHN R. THORSTENSEN Address: Department of Physics and Astronomy Dartmouth College 6127 Wilder Laboratory Hanover, NH 03755-3528; (603)-646-2869 [email protected] Undergraduate Studies: Haverford College, B. A. 1974 Astronomy and Physics double major, High Honors in both. Graduate Studies: Ph. D., 1980, University of California, Berkeley Astronomy Department Dissertation : \Optical Studies of Faint Blue X-ray Stars" Graduate Advisor: Professor C. Stuart Bowyer Employment History: Department of Physics and Astronomy, Dartmouth College: { Professor, July 1991 { present { Associate Professor, July 1986 { July 1991 { Assistant Professor, September 1980 { June 1986 Research Assistant, Space Sciences Lab., U.C. Berkeley, 1975 { 1980. Summer Student, National Radio Astronomy Observatory, 1974. Summer Student, Bartol Research Foundation, 1973. Consultant, IBM Corporation, 1973. (STARMAP program). Honors and Awards: Phi Beta Kappa, 1974. National Science Foundation Graduate Fellow, 1974 { 1977. Dorothea Klumpke Roberts Award of the Berkeley Astronomy Dept., 1978. Professional Societies: American Astronomical Society Astronomical Society of the Pacific International Astronomical Union Lifetime Publication List * \Can Collapsed Stars Close the Universe?" Thorstensen, J. R., and Partridge, R. B. 1975, Ap. J., 200, 527. \Optical Identification of Nova Scuti 1975." Raff, M. I., and Thorstensen, J. 1975, P. A. S. P., 87, 593. \Photometry of Slow X-ray Pulsars II: The 13.9 Minute Period of X Persei." Margon, B., Thorstensen, J., Bowyer, S., Mason, K. O., White, N. E., Sanford, P. W., Parkes, G., Stone, R. P. S., and Bailey, J. 1977, Ap. J., 218, 504. \A Spectrophotometric Survey of the A 0535+26 Field." Margon, B., Thorstensen, J., Nelson, J., Chanan, G., and Bowyer, S. -
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. -
Plasmas in Gamma-Ray Bursts: Particle Acceleration, Magnetic Fields, Radiative Processes and Environments
galaxies Article Plasmas in Gamma-Ray Bursts: Particle Acceleration, Magnetic Fields, Radiative Processes and Environments Asaf Pe’er Physics Department, Bar Ilan University, Ramat-Gan 52900, Israel; [email protected]; Tel.: +972-3-5318438 Received: 22 November 2018; Accepted: 7 February 2019; Published: 15 February 2019 Abstract: Being the most extreme explosions in the universe, gamma-ray bursts (GRBs) provide a unique laboratory to study various plasma physics phenomena. The complex light curve and broad-band, non-thermal spectra indicate a very complicated system on the one hand, but, on the other hand, provide a wealth of information to study it. In this chapter, I focus on recent progress in some of the key unsolved physical problems. These include: (1) particle acceleration and magnetic field generation in shock waves; (2) possible role of strong magnetic fields in accelerating the plasmas, and accelerating particles via the magnetic reconnection process; (3) various radiative processes that shape the observed light curve and spectra, both during the prompt and the afterglow phases, and finally (4) GRB environments and their possible observational signature. Keywords: jets; radiation mechanism: non-thermal; galaxies: active; gamma-ray bursts; TBD 1. Introduction Gamma-ray bursts (GRBs) are the most extreme explosions known since the big bang, releasing as much as 1055 erg (isotropically equivalent) in a few seconds, in the form of gamma rays [1]. Such a huge amount of energy released in such a short time must be accompanied by a relativistic motion of a relativistically expanding plasma. There are two separate arguments for that. First, the existence of > ± photons at energies ∼ MeV as are observed in many GRBs necessitates the production of e pairs by photon–photon interactions, as long as the optical depth for such interactions is greater than unity. -
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Spectral and Timing Analysis of the Prompt Emission of Gamma Ray Bursts A Thesis Submitted to the Tata Institute of Fundamental Research, Mumbai for the degree of Doctor of Philosophy in Physics by Rupal Basak School of Natural Sciences Tata Institute of Fundamental Research Mumbai Final Submission: Aug, 2014 arXiv:1409.5626v1 [astro-ph.HE] 19 Sep 2014 To my Parents Contents List of Publication viii 1 GRBs: The Extreme Transients 1 1.1 Overview ........................................ .............. 1 1.2 ThesisOrganization.. ... .... .... .... ... .... .... .. ................... 2 1.3 HistoryAndClassification . .................... 2 1.3.1 Discovery,AfterglowandDistanceScale . ...................... 2 1.3.2 ClassificationofGRBs . ................ 3 1.4 Observables..................................... ................ 7 1.4.1 PromptEmissionCharacteristics . ..................... 7 1.4.2 GenericFeaturesOfAfterglows . ................... 9 1.4.3 GeVEmission ................................... ............ 10 1.4.4 GRBCorrelations ............................... .............. 10 1.5 AWorkingModelforGRBs .... .... .... ... .... .... .... ................ 11 1.5.1 CompactnessAndRelativisticMotion . ..................... 11 1.5.2 “FireballModel”AndRadiationMechanism . ..................... 12 1.5.3 CentralEngineAndProgenitor. ................... 15 1.6 GRBResearch ..................................... .............. 16 1.7 BooksAndReviewArticles . .................. 17 2 Instruments And Data Analysis 18 2.1 Overview ....................................... -
The Early Optical Afterglow and Non-Thermal Components of GRB 060218
MNRAS 484, 5484–5498 (2019) doi:10.1093/mnras/stz373 Advance Access publication 2019 February 7 The early optical afterglow and non-thermal components of GRB 060218 S. W. K. Emery ,1‹ M. J. Page ,1 A. A. Breeveld,1 P. J. Brown,2 N. P. M. Kuin,1 S. R. Oates3 and M. De Pasquale4 1Mullard Space Science Laboratory, University College London, Holmbury St Mary, Dorking, Surrey RH5 6NT, UK Downloaded from https://academic.oup.com/mnras/article-abstract/484/4/5484/5308848 by University College London user on 16 April 2019 2George P. and Cynthia Woods Mitchell Institute for Fundamental Physics and Astronomy, Department of Physics and Astronomy, Texas A&M University, 4242 TAMU, College Station, TX 77843, USA 3Department of Physics, University of Warwick, Coventry CV4 7AL, UK 4Istanbul˙ University Department of Astronomy and Space Sciences, 34119 Beyazit, Istanbul,˙ Turkey Accepted 2019 February 5. Received 2018 November 13; in original form 2018 March 21 ABSTRACT We re-examine the UV/optical and X-ray observations of GRB 060218 during the prompt and afterglow phases. We present evidence in the UV/optical spectra that there is a synchrotron component contributing to the observed flux in the initial 1350 s. This result suggests that GRB 060218 is produced from a low-luminosity jet, which penetrates through its progenitor envelope after core collapse. The jet interacts with the surrounding medium to generate the UV/optical external shock synchrotron emission. After 1350 s, the thermal radiation in the UV/optical and X-ray becomes the dominant contribution to the observed flux. -