2017A&A...597A.121W


Query : 2017A&A...597A.121W

2017A&A...597A.121W - Astronomy and Astrophysics, volume 597A, 121-121 (2017/1-1)

The connection between supernova remnants and the Galactic magnetic field: An analysis of quasi-parallel and quasi-perpendicular cosmic-ray acceleration for the axisymmetric sample.

WEST J.L., SAFI-HARB S. and FERRAND G.

Abstract (from CDS):

The mechanism for the acceleration of cosmic-rays in supernova remnants (SNRs) is an outstanding question in the field. We model a sample of 32 axisymmetric SNRs using the quasi-perpendicular and quasi-parallel cosmic-ray-electron (CRE) acceleration cases. The axisymmetric sample is defined to include SNRs with a double-sided, bilateral morphology, and also those with a one-sided morphology where one limb is much brighter than the other. Using a coordinate transformation technique, we insert a bubble-like model SNR into a model of the Galactic magnetic field. Since radio emission of SNRs is dominated by synchrotron emission and since this emission depends on the magnetic field and CRE distribution, we are able to simulate the SNR emission and compare this to data. We find that the quasi-perpendicular CRE acceleration case is much more consistent with the data than the quasi-parallel CRE acceleration case, with G327.6+14.6 (SN1006) being a notable exception. We propose that SN1006 may be a case where both quasi-parallel and quasi-perpendicular acceleration are simultaneously at play in a single SNR.

Abstract Copyright: © ESO, 2017

Journal keyword(s): ISM: supernova remnants - ISM: magnetic fields - cosmic rays - radio continuum: ISM - polarization

Simbad objects: 41

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Number of rows : 41
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 SNR G119.5+10.2 SNR 00 06.6 +72 47           ~ 250 1
2 SN 1572A SN* 00 25 21.5 +64 08 27           B8 1188 1
3 SNR G127.1+00.5 SNR 01 28 20.000 +63 10 00.00           ~ 101 0
4 SNR G130.7+03.1 SNR 02 05 37.0 +64 49 42           ~ 620 4
5 1FGL J0500.1+5237 BL? 04 58 51.300 +51 50 28.00           ~ 133 1
6 AJG 116 Q? 05 26 30.000 +42 56 00.00           ~ 182 0
7 M 1 SNR 05 34 30.9 +22 00 53           ~ 6193 1
8 SNR G182.4+04.3 SNR 06 08.2 +29 00           ~ 31 0
9 SNR G189.1+02.9 SNR 06 17 01 +22 33.9           ~ 6 0
10 NAME Pup A BL? 08 24 07 -42 59.8           ~ 600 1
11 AJG 14 BL? 12 09 40 -52 25.0           ~ 287 1
12 SNR G302.3+00.7 SNR 12 45.9 -62 08           ~ 30 0
13 SNR G315.1+02.7 SNR 14 33 25.000 -57 35 30.00           ~ 25 1
14 1A 1439-61 BL? 14 43 00 -62 30.0           ~ 368 1
15 SNR G317.3-00.2 SNR 14 49.7 -59 46           ~ 19 0
16 NAME Lupus SN SNR 15 02 22.1 -42 05 49           ~ 1329 1
17 SNR G321.9-00.3 SNR 15 20 39.000 -57 33 42.00           ~ 84 0
18 SNR G327.4+01.0 SNR 15 46.8 -53 20           ~ 22 0
19 SNR G332.0+00.2 SNR 16 13.3 -50 53           ~ 47 0
20 AJG 44 Psr 16 17 33.000 -51 02 00.00           ~ 512 3
21 SNR G338.1+00.4 SNR 16 38.0 -46 24           ~ 28 0
22 SNR G356.2+04.5 SNR 17 19.0 -29 40           ~ 16 0
23 SNR G350.0-01.8 SNR 17 27 50 -38 32.0           ~ 46 0
24 SNR G354.8-00.8 SNR 17 36 00 -33 42.0           ~ 26 1
25 SNR G353.9-02.0 SNR 17 38.9 -35 11           ~ 17 0
26 SNR G359.1-00.5 Rad 17 45 30 -29 57.0           ~ 174 1
27 SNR G001.9+00.3 SNR 17 48 46.0 -27 09 52           ~ 210 1
28 SNR G003.7-00.2 SNR 17 55 26 -25 50.0           ~ 27 0
29 SNR G008.7-05.0 SNR 18 24.2 -23 48           ~ 25 0
30 SNR G016.2-02.7 SNR 18 30 00 -16 16.3           ~ 19 0
31 SNR G021.8-00.6 SNR 18 32 45 -10 08.0           ~ 129 0
32 SNR G021.6-00.8 SNR 18 33 36 -10 25.4           ~ 17 0
33 SNR G024.7-00.6 Rad 18 38 43 -07 32.0           ~ 49 1
34 SNR G028.6-00.1 Rad 18 43 55 -03 53.0           ~ 57 1
35 SNR G036.6+02.6 SNR 18 48.8 +04 26           ~ 24 0
36 SNR G042.8+00.6 SNR 19 07 41.9 +09 07 17           ~ 129 1
37 SNR G046.8-00.3 SNR 19 18 10 +12 09.0           ~ 71 0
38 SNR G054.4-00.3 SNR 19 33 20 +18 56.0           ~ 96 0
39 SNR G065.1+00.6 SNR 19 54.7 +28 35           ~ 60 0
40 SNR G093.2+06.7 SNR 20 52 25 +55 19.3           ~ 82 0
41 CTB 1 SNR 23 59 13 +62 26.2           ~ 159 0

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