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A GRB and Broad-lined Type Ic Supernova from a Single Central Engine

Jennifer BarnesColumbia Astrophysics Laboratory, Columbia University, New York, NY 10032, USA; [email protected]Paul C. DuffellDepartment of Astronomy and Theoretical Astrophysics Center, University of California, Berkeley, CA 94720, USAYu-Qian LiuCenter for Cosmology and Particle Physics, New York University, New York, NY 10003, USAM. ModjazCenter for Cosmology and Particle Physics, New York University, New York, NY 10003, USAFederica B. BiancoCenter for Cosmology and Particle Physics, New York University, New York, NY 10003, USADaniel KasenDepartment of Astronomy and Theoretical Astrophysics Center, University of California, Berkeley, CA 94720, USAAndrew MacFadyenCenter for Urban Science and Progress, New York University, Brooklyn, NY 11201, USA
2018en
ABI

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Abstract Unusually high velocities (≳0.1 c ) and correspondingly high kinetic energies have been observed in a subset of Type Ic supernovae (so-called “broad-lined Ic” supernovae; SNe Ic-BL), prompting a search for a central engine model capable of generating such energetic explosions. A clue to the explosion mechanism may lie in the fact that all supernovae that accompany long-duration gamma-ray bursts (GRBs) belong to the SN Ic-BL class. Using a combination of two-dimensional relativistic hydrodynamics and radiation transport calculations, we demonstrate that the central engine responsible for long GRBs can also trigger an SN Ic-BL. We find that a reasonable GRB engine injected into a stripped Wolf–Rayet progenitor produces a relativistic jet with energy ∼10 51 erg, as well as an SN whose synthetic light curves and spectra are fully consistent with observed SNe Ic-BL during the photospheric phase. As a result of the jet’s asymmetric energy injection, the SN spectra and light curves depend on viewing angle. The impact of viewing angle on the spectrum is particularly pronounced at early times, while the viewing-angle dependence for the light curves (∼10% variation in bolometric luminosity) persists throughout the photospheric phase.

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