2009MNRAS.397.1410T


Query : 2009MNRAS.397.1410T

2009MNRAS.397.1410T - Mon. Not. R. Astron. Soc., 397, 1410-1419 (2009/August-2)

Radio emission from supernova remnants: implications for post-shock magnetic field amplification & the magnetic fields of galaxies.

THOMPSON T.A., QUATAERT E. and MURRAY N.

Abstract (from CDS):

Using observational data from the literature, we show that the non-thermal radio luminosity (L) of supernova remnants (SNRs) is a strong function of the average gas surface density (Σg) of the galaxy in which the remnants reside, from normal spirals to dense luminous starbursts. Our result supports the interpretation of the radio sources in M82 and Arp 220 as normal SNRs, and not `radio' supernovae (SNe). We combine a simple theory for electron cooling in SNRs with their observed radio luminosities to estimate the remnant magnetic field strength (BSNR): the correlation between L and Σg implies that BSNR also increases with Σg. We explore two interpretations of this correlation: (1) BSNR is generated by post-shock magnetic field amplification, with B2SNR∝ Σgand (2) BSNR results from shock compression of the ambient interstellar medium (ISM) magnetic field (BISM), with BISM being larger in denser galaxies. We find that shock compression is, on average, sufficient to produce the observed radio emission from SNRs in the densest starburst galaxies; amplification of post-shock magnetic fields is not required. By contrast, in normal spirals modest post-shock field amplification in some remnants (a factor of ∼ few - 10) is consistent with the data; we find tentative evidence that both the Alfvén speed within SNRs and the ratio of B2SNR/8π to the post-shock pressure (`εB') are constant in SNRs from galaxy to galaxy. We discuss observational tests that can be used to more definitively distinguish between these two interpretations of the radio luminosities of SNRs. Regardless of which is correct, the radio emission from SNRs provides an upper limit to BISM that is independent of the minimum energy assumption. For the densest starbursts, the magnetic energy density in the ISM is below the total ISM pressure required for hydrostatic equilibrium; thus magnetic fields are not dynamically important on the largest scales in starbursts, in contrast with spiral galaxies like our own. This dichotomy may have implications for galactic dynamo theory.

Abstract Copyright: © 2009 The Authors. Journal compilation © 2009 RAS

Journal keyword(s): supernova remnants - galaxies: magnetic fields - galaxies: starburst - radio continuum: galaxies

Simbad objects: 27

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Number of rows : 27
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 1572A SN* 00 25 21.5 +64 08 27           B8 1254 1
2 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3588 2
3 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
4 NGC 300 GiG 00 54 53.4465638304 -37 41 03.168402396 8.83 8.69 8.13 7.46   ~ 1614 2
5 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
6 NGC 1569 rG 04 30 49.186 +64 50 52.52 11.72 11.86 11.03     ~ 1297 3
7 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
8 NGC 2146 AGN 06 18 37.710 +78 21 25.27 11.67 11.38 10.59     ~ 765 2
9 2MASS J07273756-0254540 AGN 07 27 37.5366009312 -02 54 54.264024396           ~ 69 0
10 CXOM82 J095550.9+694044 HXB 09 55 50.690 +69 40 43.76           ~ 96 0
11 M 82 AGN 09 55 52.430 +69 40 46.93 9.61 9.30 8.41     ~ 6156 6
12 NGC 3690 IG 11 28 31.0 +58 33 41   13.19 12.86     ~ 1015 4
13 M 94 SyG 12 50 53.0737971432 +41 07 12.900884628 9.15 8.96 8.24 7.78   ~ 1476 2
14 NGC 4945 Sy2 13 05 27.279 -49 28 04.44   9.31 14.40 7.55   ~ 1582 2
15 M 51 Sy2 13 29 52.698 +47 11 42.93   9.26 8.36 8.40   ~ 4565 4
16 M 83 SBG 13 37 00.91920 -29 51 56.7400 8.85 8.11 7.52 7.21   ~ 2778 2
17 ESO 134-11 HII 14 40 29 -62 38.7           ~ 585 1
18 NAME Lupus SN SNR 15 02 22.1 -42 05 49           ~ 1407 1
19 APG 220A PoG 15 34 57.22 +23 30 11.4           ~ 72 1
20 IC 1127 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 3090 4
21 APG 220B PoG 15 34 57.28 +23 30 11.3           ~ 54 1
22 LEDA 60189 LIN 17 23 21.96264 -00 17 00.8088   15.1       ~ 454 0
23 NGC 6946 H2G 20 34 52.332 +60 09 13.24   10.5       ~ 2661 2
24 SN 2000ft SN* 23 03 15.45 +08 52 26.5           SNII 40 1
25 NGC 7469 Sy1 23 03 15.6 +08 52 26 12.60 13.00 12.34     ~ 2253 3
26 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1
27 LEDA 90429 SyG 23 39 01.26960 +36 21 08.5896   16.17       ~ 232 1

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