Publication:
Fermi and Swift Observations of GRB 190114C: Tracing the Evolution of High-energy Emission from Prompt to Afterglow

dc.contributor.authorM. Ajelloen_US
dc.contributor.authorM. Arimotoen_US
dc.contributor.authorM. Axelssonen_US
dc.contributor.authorL. Baldinien_US
dc.contributor.authorG. Barbiellinien_US
dc.contributor.authorD. Bastierien_US
dc.contributor.authorR. Bellazzinien_US
dc.contributor.authorA. Berrettaen_US
dc.contributor.authorE. Bissaldien_US
dc.contributor.authorR. D. Blandforden_US
dc.contributor.authorR. Boninoen_US
dc.contributor.authorE. Bottacinien_US
dc.contributor.authorJ. Bregeonen_US
dc.contributor.authorP. Bruelen_US
dc.contributor.authorR. Buehleren_US
dc.contributor.authorE. Burnsen_US
dc.contributor.authorS. Busonen_US
dc.contributor.authorR. A. Cameronen_US
dc.contributor.authorR. Caputoen_US
dc.contributor.authorP. A. Caraveoen_US
dc.contributor.authorE. Cavazzutien_US
dc.contributor.authorS. Chenen_US
dc.contributor.authorG. Chiaroen_US
dc.contributor.authorS. Ciprinien_US
dc.contributor.authorJ. Cohen-Tanugien_US
dc.contributor.authorD. Costantinen_US
dc.contributor.authorS. Cutinien_US
dc.contributor.authorF. D'Ammandoen_US
dc.contributor.authorM. Deklotzen_US
dc.contributor.authorP. De La Torre Luqueen_US
dc.contributor.authorF. De Palmaen_US
dc.contributor.authorA. Desaien_US
dc.contributor.authorN. Di Lallaen_US
dc.contributor.authorL. Di Venereen_US
dc.contributor.authorF. Fana Dirirsaen_US
dc.contributor.authorS. J. Feganen_US
dc.contributor.authorA. Franckowiaken_US
dc.contributor.authorY. Fukazawaen_US
dc.contributor.authorS. Funken_US
dc.contributor.authorP. Fuscoen_US
dc.contributor.authorF. Garganoen_US
dc.contributor.authorD. Gasparrinien_US
dc.contributor.authorN. Gigliettoen_US
dc.contributor.authorR. Gillen_US
dc.contributor.authorF. Giordanoen_US
dc.contributor.authorM. Girolettien_US
dc.contributor.authorJ. Granoten_US
dc.contributor.authorD. Greenen_US
dc.contributor.authorI. A. Grenieren_US
dc.contributor.authorM. H. Grondinen_US
dc.contributor.authorS. Guiriecen_US
dc.contributor.authorE. Haysen_US
dc.contributor.authorD. Horanen_US
dc.contributor.authorG. Jóhannessonen_US
dc.contributor.authorD. Kocevskien_US
dc.contributor.authorM. Kovac'Evic'en_US
dc.contributor.authorM. Kussen_US
dc.contributor.authorS. Larssonen_US
dc.contributor.authorL. Latronicoen_US
dc.contributor.authorM. Lemoine-Goumarden_US
dc.contributor.authorJ. Lien_US
dc.contributor.authorI. Liodakisen_US
dc.contributor.authorF. Longoen_US
dc.contributor.authorF. Loparcoen_US
dc.contributor.authorM. N. Lovelletteen_US
dc.contributor.authorP. Lubranoen_US
dc.contributor.authorS. Malderaen_US
dc.contributor.authorD. Malysheven_US
dc.contributor.authorA. Manfredaen_US
dc.contributor.authorG. Martí-Devesaen_US
dc.contributor.authorM. N. Mazziottaen_US
dc.contributor.authorJ. E. McEneryen_US
dc.contributor.authorI. Mereuen_US
dc.contributor.authorM. Meyeren_US
dc.contributor.authorP. F. Michelsonen_US
dc.contributor.authorW. Mitthumsirien_US
dc.contributor.authorT. Mizunoen_US
dc.contributor.authorM. E. Monzanien_US
dc.contributor.authorE. Morettien_US
dc.contributor.authorA. Morsellien_US
dc.contributor.authorI. V. Moskalenkoen_US
dc.contributor.authorM. Negroen_US
dc.contributor.authorE. Nussen_US
dc.contributor.authorN. Omodeien_US
dc.contributor.authorM. Orientien_US
dc.contributor.authorE. Orlandoen_US
dc.contributor.authorM. Palatielloen_US
dc.contributor.authorV. S. Paliyaen_US
dc.contributor.authorD. Panequeen_US
dc.contributor.authorZ. Peien_US
dc.contributor.authorM. Persicen_US
dc.contributor.authorM. Pesce-Rollinsen_US
dc.contributor.authorV. Petrosianen_US
dc.contributor.authorF. Pironen_US
dc.contributor.authorH. Poonen_US
dc.contributor.authorT. A. Porteren_US
dc.contributor.authorG. Principeen_US
dc.contributor.authorJ. L. Racusinen_US
dc.contributor.authorS. Rainen_US
dc.contributor.authorR. Randoen_US
dc.contributor.otherIstituto Nazionale di Fisica Nucleare, Sezione di Triesteen_US
dc.contributor.otherIstituto Nazionale di Fisica Nucleare, Sezione di Perugiaen_US
dc.contributor.otherIstituto Nazionale di Fisica Nucleare, Sezione di Barien_US
dc.contributor.otherIstituto Nazionale di Fisica Nucleare, Sezione di Torinoen_US
dc.contributor.otherIstituto Nazionale di Fisica Nucleare, Sezione di Pisaen_US
dc.contributor.otherIstituto Nazionale Di Fisica Nucleare, Sezione di Padovaen_US
dc.contributor.otherLaboratoire Univers et Particules de Montpellieren_US
dc.contributor.otherUniversite Paris-Saclayen_US
dc.contributor.otherLaboratoire Leprince-Ringueten_US
dc.contributor.otherINAF Istituto di Astrofisica Spaziale e Fisica Cosmica, Milanen_US
dc.contributor.otherUniversity Science Institute Reykjaviken_US
dc.contributor.otherCentre d'Etudes Nucléaires de Bordeaux Gradignanen_US
dc.contributor.otherAgenzia Spaziale Italianaen_US
dc.contributor.otherHiroshima Universityen_US
dc.contributor.otherDeutsches Elektronen-Synchrotron (DESY)en_US
dc.contributor.otherOsservatorio Astronomico di Triesteen_US
dc.contributor.otherUniversità di Pisaen_US
dc.contributor.otherStockholms universiteten_US
dc.contributor.otherNaval Research Laboratoryen_US
dc.contributor.otherClemson Universityen_US
dc.contributor.otherSLAC National Accelerator Laboratoryen_US
dc.contributor.otherKanazawa Universityen_US
dc.contributor.otherUniversitat Autònoma de Barcelonaen_US
dc.contributor.otherUniversità degli Studi di Barien_US
dc.contributor.otherOpen University of Israelen_US
dc.contributor.otherIstituto Nazionale di Fisica Nucleare - INFNen_US
dc.contributor.otherUniversity of Marylanden_US
dc.contributor.otherUniversità degli Studi di Triesteen_US
dc.contributor.otherHögskolan Dalarnaen_US
dc.contributor.otherMahidol Universityen_US
dc.contributor.otherJulius-Maximilians-Universität Würzburgen_US
dc.contributor.otherIstituto Di Radioastronomia, Bolognaen_US
dc.contributor.otherUniversità degli Studi di Torinoen_US
dc.contributor.otherNASA Marshall Space Flight Centeren_US
dc.contributor.otherMax Planck Institute for Physics (Werner Heisenberg Institute)en_US
dc.contributor.otherMedizinische Universitat Innsbrucken_US
dc.contributor.otherNASA Goddard Space Flight Centeren_US
dc.contributor.otherThe George Washington Universityen_US
dc.contributor.otherUniversità degli Studi di Perugiaen_US
dc.contributor.otherThe Royal Institute of Technology (KTH)en_US
dc.contributor.otherFriedrich-Alexander-Universität Erlangen-Nürnbergen_US
dc.contributor.otherUniversity of Johannesburgen_US
dc.contributor.otherUniversità degli Studi di Padovaen_US
dc.contributor.otherStellar Solutions, Inc.en_US
dc.date.accessioned2020-05-05T05:19:34Z
dc.date.available2020-05-05T05:19:34Z
dc.date.issued2020-02-10en_US
dc.description.abstract© 2020. The American Astronomical Society.. We report on the observations of gamma-ray burst (GRB) 190114C by the Fermi Gamma-ray Space Telescope and the Neil Gehrels Swift Observatory. The prompt gamma-ray emission was detected by the Fermi GRB Monitor (GBM), the Fermi Large Area Telescope (LAT), and the Swift Burst Alert Telescope (BAT) and the long-lived afterglow emission was subsequently observed by the GBM, LAT, Swift X-ray Telescope (XRT), and Swift UV Optical Telescope. The early-time observations reveal multiple emission components that evolve independently, with a delayed power-law component that exhibits significant spectral attenuation above 40 MeV in the first few seconds of the burst. This power-law component transitions to a harder spectrum that is consistent with the afterglow emission observed by the XRT at later times. This afterglow component is clearly identifiable in the GBM and BAT light curves as a slowly fading emission component on which the rest of the prompt emission is superimposed. As a result, we are able to observe the transition from internal-shock- to external-shock-dominated emission. We find that the temporal and spectral evolution of the broadband afterglow emission can be well modeled as synchrotron emission from a forward shock propagating into a wind-like circumstellar environment. We estimate the initial bulk Lorentz factor using the observed high-energy spectral cutoff. Considering the onset of the afterglow component, we constrain the deceleration radius at which this forward shock begins to radiate in order to estimate the maximum synchrotron energy as a function of time. We find that even in the LAT energy range, there exist high-energy photons that are in tension with the theoretical maximum energy that can be achieved through synchrotron emission from a shock. These violations of the maximum synchrotron energy are further compounded by the detection of very high-energy (VHE) emission above 300 GeV by MAGIC concurrent with our observations. We conclude that the observations of VHE photons from GRB 190114C necessitates either an additional emission mechanism at very high energies that is hidden in the synchrotron component in the LAT energy range, an acceleration mechanism that imparts energy to the particles at a rate that is faster than the electron synchrotron energy-loss rate, or revisions of the fundamental assumptions used in estimating the maximum photon energy attainable through the synchrotron process.en_US
dc.identifier.citationAstrophysical Journal. Vol.890, No.1 (2020)en_US
dc.identifier.doi10.3847/1538-4357/ab5b05en_US
dc.identifier.issn15384357en_US
dc.identifier.issn0004637Xen_US
dc.identifier.other2-s2.0-85082428333en_US
dc.identifier.urihttps://repository.li.mahidol.ac.th/handle/20.500.14594/54540
dc.rightsMahidol Universityen_US
dc.rights.holderSCOPUSen_US
dc.source.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=85082428333&origin=inwarden_US
dc.subjectEarth and Planetary Sciencesen_US
dc.subjectPhysics and Astronomyen_US
dc.titleFermi and Swift Observations of GRB 190114C: Tracing the Evolution of High-energy Emission from Prompt to Afterglowen_US
dc.typeArticleen_US
dspace.entity.typePublication
mu.datasource.scopushttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=85082428333&origin=inwarden_US

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