The Spectral Sharpness Angle of Gamma-ray Bursts

We extend the results of Yu et al. (2015b) of the novel sharpness angle measurement to a large number of spectra obtained from the Fermi gamma-ray burst monitor. The sharpness angle is compared to the values obtained from various representative emission models: blackbody, single-electron synchrotr...

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Main Authors: Hendrik J. van Eerten, Jochen Greiner, Re’em Sari, P. Narayana Bhat, Andreas von Kienlin, William S. Paciesas, Robert D. Preece
Format: Article
Language:English
Published: The Korean Space Science Society 2016-06-01
Series:Journal of Astronomy and Space Sciences
Subjects:
Online Access:http://ocean.kisti.re.kr/downfile/volume/kosss/OJOOBS/2016/v33n2/OJOOBS_2016_v33n2_109.pdf
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author Hendrik J. van Eerten
Jochen Greiner
Re’em Sari
P. Narayana Bhat
Andreas von Kienlin
William S. Paciesas
Robert D. Preece
author_facet Hendrik J. van Eerten
Jochen Greiner
Re’em Sari
P. Narayana Bhat
Andreas von Kienlin
William S. Paciesas
Robert D. Preece
author_sort Hendrik J. van Eerten
collection DOAJ
description We extend the results of Yu et al. (2015b) of the novel sharpness angle measurement to a large number of spectra obtained from the Fermi gamma-ray burst monitor. The sharpness angle is compared to the values obtained from various representative emission models: blackbody, single-electron synchrotron, synchrotron emission from a Maxwellian or power-law electron distribution. It is found that more than 91% of the high temporally and spectrally resolved spectra are inconsistent with any kind of optically thin synchrotron emission model alone. It is also found that the limiting case, a single temperature Maxwellian synchrotron function, can only contribute up to 58+23 -18% of the peak flux. These results show that even the sharpest but non-realistic case, the single-electron synchrotron function, cannot explain a large fraction of the observed spectra. Since any combination of physically possible synchrotron spectra added together will always further broaden the spectrum, emission mechanisms other than optically thin synchrotron radiation are likely required in a full explanation of the spectral peaks or breaks of the GRB prompt emission phase.
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spelling doaj.art-fffbf3f860bd4dc482227592b9ab18292024-01-02T14:45:37ZengThe Korean Space Science SocietyJournal of Astronomy and Space Sciences2093-55872093-14092016-06-0133210911710.5140/JASS.2016.33.2.109The Spectral Sharpness Angle of Gamma-ray BurstsHendrik J. van Eerten0Jochen Greiner1Re’em Sari2P. Narayana Bhat3Andreas von Kienlin4William S. Paciesas5Robert D. Preece6Max Planck Institute for Extraterrestrial Physics, Garching, Bayern 85748, GermanyMax Planck Institute for Extraterrestrial Physics, Garching, Bayern 85748, GermanyThe Hebrew University of Jerusalem, Jerusalem, IsraelCenter for Space Plasma and Aeronomic Research, University of Alabama in Huntsville, Huntsville, AL 35805, USAMax Planck Institute for Extraterrestrial Physics, Garching, Bayern 85748, GermanyUniversities Space Research Association, Huntsville, AL 35805, USASpace Science Department, University of Alabama in Huntsville, Huntsville, AL 35809, USAWe extend the results of Yu et al. (2015b) of the novel sharpness angle measurement to a large number of spectra obtained from the Fermi gamma-ray burst monitor. The sharpness angle is compared to the values obtained from various representative emission models: blackbody, single-electron synchrotron, synchrotron emission from a Maxwellian or power-law electron distribution. It is found that more than 91% of the high temporally and spectrally resolved spectra are inconsistent with any kind of optically thin synchrotron emission model alone. It is also found that the limiting case, a single temperature Maxwellian synchrotron function, can only contribute up to 58+23 -18% of the peak flux. These results show that even the sharpest but non-realistic case, the single-electron synchrotron function, cannot explain a large fraction of the observed spectra. Since any combination of physically possible synchrotron spectra added together will always further broaden the spectrum, emission mechanisms other than optically thin synchrotron radiation are likely required in a full explanation of the spectral peaks or breaks of the GRB prompt emission phase.http://ocean.kisti.re.kr/downfile/volume/kosss/OJOOBS/2016/v33n2/OJOOBS_2016_v33n2_109.pdfgamma-rays: starsgamma-ray burst: generalradiation mechanisms: non-thermalradiation mechanisms: thermal
spellingShingle Hendrik J. van Eerten
Jochen Greiner
Re’em Sari
P. Narayana Bhat
Andreas von Kienlin
William S. Paciesas
Robert D. Preece
The Spectral Sharpness Angle of Gamma-ray Bursts
Journal of Astronomy and Space Sciences
gamma-rays: stars
gamma-ray burst: general
radiation mechanisms: non-thermal
radiation mechanisms: thermal
title The Spectral Sharpness Angle of Gamma-ray Bursts
title_full The Spectral Sharpness Angle of Gamma-ray Bursts
title_fullStr The Spectral Sharpness Angle of Gamma-ray Bursts
title_full_unstemmed The Spectral Sharpness Angle of Gamma-ray Bursts
title_short The Spectral Sharpness Angle of Gamma-ray Bursts
title_sort spectral sharpness angle of gamma ray bursts
topic gamma-rays: stars
gamma-ray burst: general
radiation mechanisms: non-thermal
radiation mechanisms: thermal
url http://ocean.kisti.re.kr/downfile/volume/kosss/OJOOBS/2016/v33n2/OJOOBS_2016_v33n2_109.pdf
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