2018MNRAS.479.4470M


Query : 2018MNRAS.479.4470M

2018MNRAS.479.4470M - Mon. Not. R. Astron. Soc., 479, 4470-4485 (2018/October-0)

Core-collapse supernovae as cosmic ray sources.

MARCOWITH A., DWARKADAS V.V., RENAUD M., TATISCHEFF V. and GIACINTI G.

Abstract (from CDS):

Core-collapse supernovae produce fast shocks which pervade the dense circumstellar medium (CSM) of the stellar progenitor. Cosmic rays (CRs) if accelerated at these shocks can induce the growth of electromagnetic fluctuations in the foreshock medium. In this study, using a self-similar description of the shock evolution, we calculate the growth time-scales of CR-driven instabilities. We select a sample of nearby core-collapse radio supernova of type II and Ib/Ic. From radio data, we infer the parameters which enter in the calculation of the instability growth times. We find that extended IIb SNe shocks can trigger fast intra-day instabilities, strong magnetic field amplification, and CR acceleration. In particular, the non-resonant streaming instability can contribute to about 50 per cent of the magnetic field intensity deduced from radio data. This results in the acceleration of CRs in the range 1-10 PeV within a few days after the shock breakout. In order to produce strong magnetic field amplification and CR acceleration, a fast shock pervading a dense CSM is necessary. In that aspect, IIn supernovae are also good candidates. But a detailed modelling of the blast wave dynamics coupled with particle acceleration is mandatory for this class of object before providing any firm conclusions. Finally, we find that the trans-relativistic object SN 2009bb even if it produces more modest magnetic field amplification can accelerate CRs up to 2-3 PeV within 20 d after the outburst.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): acceleration of particles - shock waves - cosmic rays

Simbad objects: 26

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Number of rows : 26
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 2002ic SN* 01 30 02.55 +21 53 06.9     18.5     SNIapec 252 1
2 SN 1986J SN* 02 22 31.33 +42 19 56.4   18.4 18.4     SNII 331 1
3 SN 2005kd SN* 04 03 16.88 +71 43 18.9     17.0     SNIIn 48 1
4 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
5 * alf Ori s*r 05 55 10.30536 +07 24 25.4304 4.38 2.27 0.42 -1.17 -2.45 M1-M2Ia-Iab 1789 0
6 HD 50896 WR* 06 54 13.0439608392 -23 55 42.023319852 5.74 6.63 6.91 7.74   WN4b 794 0
7 V* VY CMa s*r 07 22 58.3261352189 -25 46 03.194390594 12.01 10.068 8.691 7.938   M5Iae 1169 0
8 SN 2006jc SN* 09 17 20.78 +41 54 32.7     13.8     SNIbn 380 1
9 SN 2010jl SN* 09 42 53.33 +09 29 41.8           SNIIn 350 1
10 SN 1997ab SN* 09 51 00.212 +20 04 19.88   14.7       SNIIn 60 1
11 SN 1993J SN* 09 55 24.77476 +69 01 13.7026   10.8 12.0     SNIIb 1507 1
12 M 81 Sy2 09 55 33.1726556496 +69 03 55.062505368   7.89 6.94     ~ 4725 3
13 SN 2008iz SN* 09 55 51.55 +69 40 45.8           SNII: 63 1
14 SN 2009bb SN* 10 31 33.92 -39 57 28.2           SNIc 185 1
15 SN 2003L SN* 11 03 12.33 +11 04 38.3     16.9     SNIc 77 1
16 SN 1998S SN* 11 46 06.1 +47 28 55     12.2     SNIIn 517 1
17 SN 1979C SN* 12 22 58.58 +15 47 52.7   11.6       SNIIL 609 1
18 SN 2008ax SN* 12 30 40.80 +41 38 16.1   23.6 23.5 14.1 22.6 SNIIb 295 1
19 SN 1997eg SN* 13 11 36.73 +22 55 29.4     15.6     SNIIn 78 1
20 SN 2001gd SN* 13 13 23.89 +36 38 17.7     16.5     SNIIb 62 1
21 SN 1994I SN* 13 29 54.072 +47 11 30.50     12.9     SNIc 645 1
22 SN 2011dh SN* 13 30 05.10555 +47 10 10.9227           SNIIb 445 1
23 SN 1983N SN* 13 36 51.23 -29 54 01.7   11.7       SNIb 278 1
24 SN 1996cr SN* 14 13 10.01139 -65 20 44.5654     19.5     SNIIn: 90 1
25 SN 1995N SN* 14 49 28.29 -10 10 14.0     17.5     SNIIn 172 1
26 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1

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