4.6 Article

The Swift/Fermi GRB 080928 from 1 eV to 150 keV

期刊

ASTRONOMY & ASTROPHYSICS
卷 529, 期 -, 页码 -

出版社

EDP SCIENCES S A
DOI: 10.1051/0004-6361/201015324

关键词

gamma-ray burst: individual: GRB 080928

资金

  1. DFG [K1 766/11-3, K1 766/16-1, HA 1850/28-1]
  2. BLANCEFLOR Boncompagni-Ludovisi, nee Bildt foundation
  3. Thuringer Landessternwarte Tautenburg, Germany
  4. Icelandic Research Fund
  5. Science and Technology Facilities Council [ST/H00243X/1, PP/C002229/1, ST/H004157/1, ST/H004165/1] Funding Source: researchfish
  6. STFC [ST/H004157/1, ST/H004165/1, PP/C002229/1] Funding Source: UKRI
  7. Direct For Mathematical & Physical Scien
  8. Division Of Physics [801007] Funding Source: National Science Foundation

向作者/读者索取更多资源

We present the results of a comprehensive study of the gamma-ray burst 080928 and of its afterglow. GRB 080928 was a long burst detected by Swift/BAT and Fermi/GBM. It is one of the exceptional cases where optical emission had already been detected when the GRB itself was still radiating in the gamma-ray band. For nearly 100 s simultaneous optical, X-ray and gamma-ray data provide a coverage of the spectral energy distribution of the transient source from about 1 eV to 150 keV. In particular, we show that the SED during the main prompt emission phase agrees with synchrotron radiation. We constructed the optical/near-infrared light curve and the spectral energy distribution based on Swift/UVOT, ROTSE-IIIa (Australia), and GROND (La Silla) data and compared it to the X-ray light curve retrieved from the Swift/XRT repository. We show that its bumpy shape can be modeled by multiple energy-injections into the forward shock. Furthermore, we investigate whether the temporal and spectral evolution of the tail emission of the first strong flare seen in the early X-ray light curve can be explained by large-angle emission (LAE). We find that a nonstandard LAE model is required to explain the observations. Finally, we report on the results of our search for the GRB host galaxy, for which only a deep upper limit can be provided.

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