2020ApJ...900..193D


Query : 2020ApJ...900..193D

2020ApJ...900..193D - Astrophys. J., 900, 193-193 (2020/September-2)

How dense of a circumstellar medium is sufficient to choke a jet?

DUFFELL P.C. and HO A.Y.Q.

Abstract (from CDS):

The progenitor stars of stripped-envelope high-velocity supernovae (Ic-BL SNe) can explode inside a dense circumstellar medium (CSM) that extends out to many times the progenitor radius. This complicates the question of whether all Ic-BL SNe harbor a jet, which can tunnel through the star and be viewed on-axis as a long-duration gamma-ray burst (GRB). More specifically, a sufficiently dense CSM might "choke" the jet, redistributing its energy quasi-spherically. In this study, we numerically calculate the CSM density necessary for jet choking. For typical GRBs, we determine the jet is not choked in the CSM unless ρr2> 4×1019gcm–1; this requires several solar masses of CSM to be situated within 1013 cm of the progenitor, a much higher density than any CSM observed. We conclude that typical GRB jets are not choked in the CSM. However, in many cases the CSM has sufficient mass to decelerate the jet to a modest Lorentz factor (Γ ∼ 10), which should lead to a long coasting phase for the jet, observable as a long plateau (potentially up to a few days) in the afterglow light curve. For extreme cases of low-energy GRBs in a high-mass CSM, the jet will decelerate to nonrelativistic velocities, causing it to spread modestly to a larger opening angle (θj ≃ 20°) before breaking out of the CSM. Even in these extreme examples, the jet does not have time to redistribute its energy quasi-spherically in the CSM before breakout.

Abstract Copyright: © 2020. The American Astronomical Society. All rights reserved.

Journal keyword(s): Circumstellar matter - Supernovae - Relativistic jets - Relativistic fluid dynamics - Gamma-ray bursts

Simbad objects: 8

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Number of rows : 8
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
2 SN 2003L SN* 11 03 12.33 +11 04 38.3     16.9     SNIc 77 1
3 SN 2017iuk SN* 11 09 39.49 -12 35 18.7           SNII 210 0
4 SN 2007bg SN* 11 49 26.18 +51 49 21.8 20.1 19.8 18.8     SNIc-BL 72 1
5 iPTF 16asu SN* 12 59 09.28 +13 48 09.2           SLSN-I 49 0
6 PTF 11qcj SN* 13 13 41.51 +47 17 57.0           SNIb 62 0
7 SN 2018gep SN* 16 43 48.2 +41 02 43           SNIc-BL 66 0
8 SN 2016coi SN* 21 59 04.14 +18 11 10.5           SNIc 67 0

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