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LOW-RESOLUTION SPECTROSCOPY OF GAMMA-RAY BURST OPTICAL AFTERGLOWS: BIASES IN THE <i>SWIFT</i> SAMPLE AND CHARACTERIZATION OF THE ABSORBERS

J. P. U. FynboDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen Ø, DenmarkP. JakobssonCentre for Astrophysics and Cosmology, Science Institute, University of Iceland, Dunhagi 5, IS‐107 Reykjavik, IcelandJ. X. ProchaskaDepartment of Astronomy and Astrophysics, UCO/Lick Observatory; University of California, 1156 High Street, Santa Cruz, CA 95064, USAD. MalesaniDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen Ø, Denmark ,C. LedouxEuropean Southern Observatory, Alonso de Córdova 3107, Vitacura Casilla 19001, Santiago 19, ChileA. de Ugarte PostigoEuropean Southern Observatory, Alonso de Córdova 3107, Vitacura Casilla 19001, Santiago 19, ChileM. NardiniSISSA, via Beirut, 2-4, I-34014, Trieste,#N#Italy#N#P. M. VreeswijkEuropean Southern Observatory, Alonso de Córdova 3107, Vitacura, Casilla 19001, Santiago 19, ChileK. WiersemaDepartment of Physics & Astronomy,University of Leicester,University Road,Leicester,LE1 7RH,UKJ. HjorthDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen Ø, Denmark ,J. SollermanDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen Ø, DenmarkHsiao‐Wen ChenDepartment of Astronomy & Astrophysics, and Kavli Institute for Cosmological Physics, University of Chicago, Chicago, IL 60637, USAC. C. ThöneDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen O, DenmarkG. BjörnssonCentre for Astrophysics and Cosmology, Science Institute, University of Iceland, Dunhagi 5, IS‐107 Reykjavik, IcelandJ. S. BloomDepartment of Astronomy, University of California, Berkeley, CA, 94720-3411, USAA. J. Castro‐TiradoIAA-CSIC, P.O. Box 03004, E-18080 Granada, SpainL. ChristensenEuropean Southern Observatory, Karl-Schwarzschildstrasse 2,#N#D-85748 Garching, GermanyA. DeCentre for Astrophysics and Cosmology, Science Institute, University of Iceland, Dunhagi 5, IS‐107 Reykjavik, IcelandA. S. FruchterSpace Telescope Science Institute, Department of Physics and Astronomy, Johns Hopkins University, 3700 San Martin Drive, Baltimore, MD 21218, USAJ. GorosabelIAA-CSIC, P.O. Box 03004, E-18080 Granada, SpainJ. F. GrahamSpace Telescope Science Institute, Department of Physics and Astronomy, Johns Hopkins University, 3700 San Martin Drive, Baltimore, MD 21218, USAA. O. JaunsenDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen Ø, DenmarkB. L. JensenDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen Ø, Denmark ,Д. А. КаннThüringer Landessternwarte Tautenburg, Sternwarte 5, D-07778 Tautenburg, GermanyC. KouveliotouNASA Marshall Space Flight Center, Huntsville, AL 35805, USA#TAB#A. J. LevanDepartment of Physics, University of Warwick, Coventry CV4 7AL, UKJustyn R. MaundDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen Ø, Denmark ,N. MasettiINAF – Istituto di Astrofisica Spaziale e Fisica Cosmica di Bologna, via Gobetti 101, 40129 Bologna, ItalyB. Milvang‐JensenDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen Ø, Denmark ,E. PalazziINAF – Istituto di Astrofisica Spaziale e Fisica Cosmica di Bologna, via Gobetti 101, 40129 Bologna, ItalyD. A. PerleyDepartment of Astronomy, University of California, Berkeley, CA, 94720-3411, USAE. PianINAF—Trieste Astronomical Observatory, 34143 Trieste, ItalyE. RolDepartment of Physics & Astronomy,University of Leicester,University Road,Leicester,LE1 7RH,UKP. SchadyR. L. C. StarlingDepartment of Physics & Astronomy,University of Leicester,University Road,Leicester,LE1 7RH,UKN. R. TanvirDepartment of Physics & Astronomy,University of Leicester,University Road,Leicester,LE1 7RH,UKD. WatsonDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen Ø, Denmark ,D. XuDark Cosmology Centre, Niels Bohr Institute, University of Copenhagen, Juliane Maries Vej 30, DK-2100 Copenhagen Ø, Denmark ,T. AugusteijnNordic Optical Telescope Apartado 474, 38700 Santa Cruz de La Palma, Santa Cruz de Tenerife, SpainF. GrundahlJ. H. TeltingNordic Optical Telescope Apartado 474, 38700 Santa Cruz de La Palma, Santa Cruz de Tenerife, SpainPierre-Olivier Quirion
2009en
ABI

Аннотация

We present a sample of 77 optical afterglows (OAs) of Swift detected gamma-ray bursts (GRBs) for which spectroscopic follow-up observations have been secured. Our first objective is to measure the redshifts of the bursts. For the majority (90%) of the afterglows, the redshifts have been determined from the spectra. We provide line lists and equivalent widths (EWs) for all detected lines redward of Lyα covered by the spectra. In addition to the GRB absorption systems, these lists include line strengths for a total of 33 intervening absorption systems. We discuss to what extent the current sample of Swift bursts with OA spectroscopy is a biased subsample of all Swift detected GRBs. For that purpose we define an X-ray-selected statistical sample of Swift bursts with optimal conditions for ground-based follow-up from the period 2005 March to 2008 September; 146 bursts fulfill our sample criteria. We derive the redshift distribution for the statistical (X-ray selected) sample and conclude that less than 18% of Swift bursts can be at z &gt; 7. We compare the high-energy properties (e.g., y-ray (15-350 keV) fluence and duration, X-ray flux, and excess absorption) for three subsamples of bursts in the statistical sample: (1) bursts with redshifts measured from OA spectroscopy; (2) bursts with detected optical and/or near-IR afterglow, but no afterglow-based redshift; and (3) bursts with no detection of the OA. The bursts in group (1) have slightly higher y-ray fluences and higher X-ray fluxes and significantly less excess X-ray absorption than bursts in the other two groups. In addition, the fractions of dark bursts, defined as bursts with an optical to X-ray slope fox &lt; 0.5, is 14% in group (1), 38% in group (2), and &gt;39% in group (3). For the full sample, the dark burst fraction is constrained to be in the range 25%-42%. From this we conclude that the sample of GRBs with OA spectroscopy is not representative for all Swift bursts, most likely due to a bias against the most dusty sight lines. This should be taken into account when determining, e.g., the redshift or metallicity distribution of GRBs and when using GRBs as a probe of star formation. Finally, we characterize GRB absorption systems as a class and compare them to QSO absorption systems, in particular the damped Lyα absorbers (DLAs). On average GRB absorbers are characterized by significantly stronger EWs for Hi as well as for both low and high ionization metal lines than what is seen in intervening QSO absorbers. However, the distribution of line strengths is very broad and several GRB absorbers have lines with EWs well within the range spanned by QSO-DLAs. Based on the 33 z &gt; 2 bursts in the sample, we place a 95% confidence upper limit of 7.5% on the mean escape fraction of ionizing photons from star-forming galaxies. © 2009 T'he American Astronomical Society.

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