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dc.contributor.authorDe Colle, Fabio
dc.contributor.authorGranot, Jonathan
dc.contributor.authorLopez-Camara, Diego
dc.contributor.authorRamirez-Ruiz, Enrico
dc.date.accessioned2012-03-27T08:00:40Z
dc.date.available2012-03-27T08:00:40Z
dc.date.issued2012-02-20
dc.identifier.citationDe Colle , F , Granot , J , Lopez-Camara , D & Ramirez-Ruiz , E 2012 , ' Gamma-ray burst dynamics and afterglow radiation from adaptive mesh refinement, special relativistic hydrodynamic simulations. ' , The Astrophysical Journal , vol. 746 , no. 2 , 122 . https://doi.org/10.1088/0004-637X/746/2/122
dc.identifier.issn0004-637X
dc.identifier.urihttp://hdl.handle.net/2299/8056
dc.description.abstractWe report on the development of Mezcal-SRHD, a new adaptive mesh refinement, special relativistic hydrodynamics (SRHD) code, developed with the aim of studying the highly relativistic flows in gamma-ray burst sources. The SRHD equations are solved using finite-volume conservative solvers, with second-order interpolation in space and time. The correct implementation of the algorithms is verified by one-dimensional (1D) and multi-dimensional tests. The code is then applied to study the propagation of 1D spherical impulsive blast waves expanding in a stratified medium with rho proportional to r (k), bridging between the relativistic and Newtonian phases (which are described by the Blandford-McKee and Sedov-Taylor self-similar solutions, respectively), as well as to a two-dimensional (2D) cylindrically symmetric impulsive jet propagating in a constant density medium. It is shown that the deceleration to nonrelativistic speeds in one dimension occurs on scales significantly larger than the Sedov length. This transition is further delayed with respect to the Sedov length as the degree of stratification of the ambient medium is increased. This result, together with the scaling of position, Lorentz factor, and the shock velocity as a function of time and shock radius, is explained here using a simple analytical model based on energy conservation. The method used for calculating the afterglow radiation by post-processing the results of the simulations is described in detail. The light curves computed using the results of 1D numerical simulations during the relativistic stage correctly reproduce those calculated assuming the self-similar Blandford-McKee solution for the evolution of the flow. The jet dynamics from our 2D simulations and the resulting afterglow light curves, including the jet break, are in good agreement with those presented in previous works. Finally, we show how the details of the dynamics critically depend on properly resolving the structure of the relativistic flow.en
dc.format.extent18
dc.format.extent3610495
dc.language.isoeng
dc.relation.ispartofThe Astrophysical Journal
dc.subjectgamma-ray burst: general
dc.subjecthydrodynamics
dc.subjectmethods: numerical
dc.subjectradiation mechanisms: non-thermal
dc.subjectrelativistic processes
dc.subjectshock waves
dc.subjectEQUATION-OF-STATE
dc.subjectMAGNETIC-FIELD AMPLIFICATION
dc.subjectCOALESCING NEUTRON-STARS
dc.subjectROTATING BLACK-HOLE
dc.subjectLIGHT CURVES
dc.subjectMAGNETOHYDRODYNAMIC SIMULATIONS
dc.subjectFERMI OBSERVATIONS
dc.subjectACCRETION DISKS
dc.subjectMASSIVE STARS
dc.subjectJET FORMATION
dc.titleGamma-ray burst dynamics and afterglow radiation from adaptive mesh refinement, special relativistic hydrodynamic simulations.en
dc.contributor.institutionSchool of Physics, Astronomy and Mathematics
dc.contributor.institutionScience & Technology Research Institute
dc.contributor.institutionCentre for Astrophysics Research
dc.description.statusPeer reviewed
rioxxterms.versionofrecord10.1088/0004-637X/746/2/122
rioxxterms.typeJournal Article/Review
herts.preservation.rarelyaccessedtrue


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