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 "title": "GRB 050820A",
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 "excerpt": "GRB 050820A was an exceptionally energetic long gamma-ray burst detected by Swift on 20 August 2005 at redshift 2.612, with one of the Swift era's best-sampled broadband data sets.",
 "snippet": "GRB 050820A was an exceptionally energetic long gamma-ray burst detected by Swift on 20 August 2005 at redshift 2.612, with one of the Swift era's best-sampled broadband data sets.",
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 "markdown": "# GRB 050820A\n\n**GRB 050820A** was a long, exceptionally energetic gamma-ray burst detected by the Swift Burst Alert Telescope on 20 August 2005 at 06:34:53 UTC (trigger 151207), at a redshift of 2.612 measured from absorption lines with Keck and 2.6147 with VLT.<sup>[1](https://swift.gsfc.nasa.gov/archive/grb_table/grb_lookup.php?grb_name=050820A)</sup> It is one of the best-sampled broadband data sets of the Swift era, followed simultaneously in gamma-ray, X-ray, and optical bands thanks to a soft precursor pulse about 200 seconds before the main event.<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup> Its prompt gamma-ray energy release and afterglow kinetic energy make it one of the most energetic events for which such values could be determined.<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup>\n\n| Key fact | Detail |\n|---|---|\n| Detection | Swift BAT trigger 151207, 20 August 2005, 06:34:53 UTC; BAT T90 = 26 s, fluence 34.40 × 10<sup>−7</sup> erg cm<sup>−2</sup> (15–150 keV)<sup>[1](https://swift.gsfc.nasa.gov/archive/grb_table/grb_lookup.php?grb_name=050820A)</sup> |\n| Distance | Redshift 2.612 (Keck absorption); 2.6147 (VLT absorption)<sup>[1](https://swift.gsfc.nasa.gov/archive/grb_table/grb_lookup.php?grb_name=050820A)</sup> |\n| Precursor | Soft gamma-ray pulse about 200 s before the main event, with no intervening emission, suggesting a mechanism distinct from the GRB itself<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup> |\n| Prompt energy | E<sub>γ,iso</sub> = (9.7<sup>+3.1</sup><sub>−1.4</sub>) × 10<sup>53</sup> erg in a 1–10<sup>4</sup> MeV rest-frame bandpass, from a Konus/Wind fluence of (6.1<sup>+1.9</sup><sub>−0.9</sub>) × 10<sup>−5</sup> erg cm<sup>−2</sup><sup> • </sup><sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup> |\n| Collimation | Jet opening angle θ = 6.8–9.3 degrees from an achromatic jet break seen between about 7 and 36 days<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup> |\n| Calorimetry | Afterglow kinetic energy E<sub>KE</sub> = 5.2<sup>+7.9</sup><sub>−4.1</sub> × 10<sup>51</sup> erg; beaming-corrected prompt energy E<sub>γ</sub> = 7.5<sup>+6.7</sup><sub>−2.4</sub> × 10<sup>51</sup> erg<sup>[4](https://pure.psu.edu/en/publications/multiwavelength-observations-of-grb-050820a-an-exceptionally-ener/)</sup> |\n| Early optical | Optical and X-ray emission brightened abruptly at t ≈ 220 s in step with the gamma-ray rise; interpreted by the Vestrand team as a reverberation of the prompt energy input<sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup><sup> • </sup><sup>[5](https://www.nature.com/articles/nature04913)</sup> |\n\n## Detection and prompt emission\n\nSwift's [Burst Alert Telescope](https://www.edgepedia.org/burst-alert-telescope) triggered on a faint gamma-ray precursor nearly 4 minutes before the bulk of the prompt emission.<sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup> The gamma-ray light curve is marked by this soft precursor pulse some 200 s before the main event; the lack of any intervening emission suggests it is due to a physical mechanism distinct from the GRB itself.<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup> The large time lag between precursor and main event enabled simultaneous observations in the gamma-ray, X-ray, and optical bandpasses, something achieved for only a handful of events at that time.<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup>\n\nThe prompt emission was observed by the Konus/[Wind instrument](https://www.edgepedia.org/wind-instrument) with spectral coverage from 20 keV to 1 MeV.<sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup> Extrapolating the observed spectrum to a rest-frame bandpass of 1–10<sup>4</sup> MeV gives a fluence of (6.1<sup>+1.9</sup><sub>−0.9</sub>) × 10<sup>−5</sup> erg cm<sup>−2</sup>, and at z = 2.615 an isotropic prompt energy release of E<sub>γ,iso</sub> = (9.7<sup>+3.1</sup><sub>−1.4</sub>) × 10<sup>53</sup> erg.<sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup> Among the bursts in a comparative sample, GRB 050820A had the largest prompt energy.\n\n## Early optical emission and the reverberation interpretation\n\nThe event settled a question about when the early afterglow begins. Optical emission in the first minutes after a burst had been sorted into two classes: prompt optical emission correlated with the prompt gamma rays, and early optical afterglow emission uncorrelated with them.<sup>[5](https://www.nature.com/articles/nature04913)</sup> Observations of GRB 050820A, principally with the RAPTOR telescope at [Los Alamos National Laboratory](https://www.edgepedia.org/los-alamos-national-laboratory), showed for the first time the temporal relationship and relative strength of the two optical components.<sup>[5](https://www.nature.com/articles/nature04913)</sup>\n\nBoth the X-ray and the optical emission brightened abruptly in concert with the onset of the main gamma-ray episode at t ≈ 220 s, suggesting a common origin.<sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup> The contemporaneous X-rays are the low-energy tail of the prompt emission, but the optical does not directly track the gamma-ray flux; the early optical data instead appear consistent with the forward-shock synchrotron peak passing through the optical band, and are therefore likely the beginning of the afterglow.<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup> The Vestrand team interpreted the early afterglow as a reverberation of the energy input measured by the prompt emission, meaning the early afterglow does not begin at the trigger time as normally assumed.<sup>[5](https://www.nature.com/articles/nature04913)</sup> Because such reverberations probe the structure of the environment around the burst, and because many long GRBs come from massive stars that died when the [Universe](https://www.edgepedia.org/universe) was less than ten per cent of its current age, they offer clues about the environments around some of the first stars.<sup>[5](https://www.nature.com/articles/nature04913)</sup>\n\n## Afterglow behavior and energy injection\n\nOn hour timescales the X-ray and optical light curves are inconsistent with a simple adiabatic expansion of the shock into the surrounding medium and instead indicate a period of energy injection.<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup> The radio light curve shows a bright flare at t ≈ 1 day that is probably reverse-shock emission.<sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup> A later decomposition of Swift-era light curves found that the X-ray emission of GRB 050820A is dominated by a \"late prompt\" component up to 200 ks in the rest frame (720 ks in the observer frame), with the standard afterglow taking over after that; in the optical, the standard afterglow prevails throughout except around 5 ks rest frame (18 ks observer frame), where the two contributions become comparable.<sup>[6](https://academic.oup.com/mnras/article/403/3/1131/1046479)</sup>\n\nThe afterglow was bright enough that its decay could be traced to late times, including [Hubble Space Telescope](https://www.edgepedia.org/hubble-space-telescope) observations at t ≈ 36 days.<sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup> The optical light curve shows a distinct break between the last ground-based detection at t ≈ 7 days and those HST observations, and late-time X-ray data establish the same break in the X-ray band, identifying it as a jet break.<sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup>\n\n## Energetics and jet collimation\n\nThe jet break constrains the collimation angle of the relativistic outflow to θ = 6.8–9.3 degrees.<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup> Correcting the isotropic energy for beaming gives a prompt energy release of E<sub>γ</sub> = 7.5<sup>+6.7</sup><sub>−2.4</sub> × 10<sup>51</sup> erg, alongside an afterglow kinetic energy of E<sub>KE</sub> = 5.2<sup>+7.9</sup><sub>−4.1</sub> × 10<sup>51</sup> erg.<sup>[4](https://pure.psu.edu/en/publications/multiwavelength-observations-of-grb-050820a-an-exceptionally-ener/)</sup> Together these make GRB 050820A one of the most energetic events for which such values could be determined.<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup>\n\nModeling of the afterglow found that no high-quality fits were possible assuming a wind-like circumburst medium.<sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup> In a 2022 broadband reanalysis using the afterglowpy forward-shock code, the jet was found to be nearly a top-hat structure, with a half opening angle of only about 0.015 rad and a circumburst medium density as low as 10<sup>−7</sup> cm<sup>−3</sup>; the authors interpret this as evidence for a metal-poor progenitor star that lost mass at a low rate.<sup>[7](https://www.raa-journal.org/issues/all/2022/v22n8/202208/P020220805559622102403.pdf)</sup>\n\n## Significance\n\nGRB 050820A served as a test case for afterglow theory in several ways at once. Its delayed main event produced one of the few simultaneous gamma-ray, X-ray, and optical records of a burst's first minutes, showing that the early afterglow can begin as a response to prompt energy release rather than at trigger time.<sup>[2](https://arxiv.org/abs/astro-ph/0608183)</sup><sup> • </sup><sup>[5](https://www.nature.com/articles/nature04913)</sup> Its clear achromatic jet break contributed to the evidence that bright Swift bursts are collimated explosions, while the large opening angles found for such events argued against a strictly canonical energy release of about 10<sup>51</sup> erg for all GRBs.<sup>[3](https://doi.org/10.1088/0004-637X/711/2/641)</sup> Its high redshift and abundant multi-wavelength afterglow data have kept it a reference event for jet-structure modeling.<sup>[7](https://www.raa-journal.org/issues/all/2022/v22n8/202208/P020220805559622102403.pdf)</sup>\n\n## References\n\n1. [GRB 050820A, Swift GRB table, NASA Goddard Space Flight Center](https://swift.gsfc.nasa.gov/archive/grb_table/grb_lookup.php?grb_name=050820A)\n2. [Cenko, S. B. et al. (2006). Multi-Wavelength Observations of GRB 050820A: An Exceptionally Energetic Event Followed from Start to Finish. arXiv:astro-ph/0608183](https://arxiv.org/abs/astro-ph/0608183)\n3. [Cenko, S. B. et al. (2010). The Collimation and Energetics of the Brightest Swift Gamma-Ray Bursts. The Astrophysical Journal 711, 641](https://doi.org/10.1088/0004-637X/711/2/641)\n4. [Multiwavelength observations of GRB 050820A, Penn State research portal](https://pure.psu.edu/en/publications/multiwavelength-observations-of-grb-050820a-an-exceptionally-ener/)\n5. [Vestrand, W. T. et al. (2006). Energy input and response from prompt and early optical afterglow emission in γ-ray bursts. Nature 442, 172–175](https://www.nature.com/articles/nature04913)\n6. [Testing a new view of gamma-ray burst afterglows. Monthly Notices of the Royal Astronomical Society 403, 1131](https://academic.oup.com/mnras/article/403/3/1131/1046479)\n7. [Li, X.-Y., He, H.-N., & Wei, D.-M. (2022). On the Jet Structures of GRB 050820A and GRB 070125. Research in Astronomy and Astrophysics 22, 085021](https://www.raa-journal.org/issues/all/2022/v22n8/202208/P020220805559622102403.pdf)\n\n---\n*Topic: Encyclopedia › Physical world and mathematics › Astronomy › Stars and galaxies › Compact objects, supernovae, and remnants*\n\n*Initially written Oct 15, 2026*\n\n*Copyright 2026 EdgeChat AI, a subsidiary of Biostate AI.*\n\nLicense: Edgepedia Community License 1.0, https://www.edgepedia.org/edgepedia/license\n",
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 "credit": "\"GRB 050820A\", Edgepedia (EdgeChat), https://www.edgepedia.org/grb-050820a. Edgepedia Community License 1.0.",
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 "speakable": "GRB 050820A was an exceptionally energetic long gamma-ray burst detected by Swift on 20 August 2005 at redshift 2.612, with one of the Swift era's best-sampled broadband data sets."
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