2021ApJ...907....2S


Query : 2021ApJ...907....2S

2021ApJ...907....2S - Astrophys. J., 907, 2-2 (2021/January-3)

Magnetic fields in elliptical galaxies: an observational probe of the fluctuation dynamo action.

SETA A., RODRIGUES L.F.S., FEDERRATH C. and HALES C.A.

Abstract (from CDS):

Fluctuation dynamos are thought to play an essential role in the evolution of magnetized galaxies, saturating within ∼0.01 Gyr and thus potentially acting as seeds for large-scale mean-field dynamos. However, unambiguous observational confirmation of the fluctuation dynamo action in a galactic environment is still missing. This is because, in spiral galaxies, it is difficult to differentiate between small-scale magnetic fields generated by a fluctuation dynamo and those due to the tangling of the large-scale field. We propose that observations of magnetic fields in elliptical galaxies would directly probe the fluctuation dynamo action. This is motivated by the fact that in ellipticals, due to their lack of significant rotation, the conventional large-scale dynamo is absent and the fluctuation dynamo is responsible for controlling the strength and structure of the magnetic field. By considering turbulence injected by Type Ia supernova explosions and possible magnetic field amplification by cooling flows, we estimate expected magnetic field strengths of 0.2–1µG in the centers of quiescent elliptical galaxies. We use a semianalytic model of galaxy formation to estimate the distribution and redshift evolution of field strengths, tentatively finding a decrease in magnetic field strength with decreasing redshift. We analyze a historical sample of radio sources that exhibit the Laing-Garrington effect (radio polarization asymmetry in jets) and infer magnetic field strengths between 0.14and1.33µG for a uniform thermal electron density and between 1.36and6.21µG for the thermal electron density following the King profile. We examine observational techniques for measuring the magnetic field saturation state in elliptical galaxies, focusing on Faraday rotation measure grids, the Laing-Garrington effect, synchrotron emission, and gravitational lensing, and finding appealing prospects for future empirical analysis.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Galaxy magnetic fields - Elliptical galaxies - Interstellar magnetic fields - Polarimetry - Magnetic fields

Simbad objects: 34

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Number of rows : 34
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 3C 9 BLL 00 20 25.2231670656 +15 40 54.774271884   17.92 17.62     ~ 347 1
2 3C 34.0 rG 01 10 18.665 +31 47 20.48   21       ~ 177 2
3 3C 41.0 rG 01 26 44.388 +33 13 11.22   21       ~ 172 1
4 4C -01.11 QSO 02 28 07.8477815280 -01 15 40.318943400     18.00     ~ 94 2
5 4C -04.06 QSO 02 35 07.3418452008 -04 02 05.317096956   16.61 16.46 16.2   ~ 222 1
6 UGCA 34 GiG 02 36 35.4662282832 +59 39 17.507008584   17       ~ 198 2
7 4C 53.16 rG 07 16 41.2170214056 +53 23 09.555141120   14.55 14.0     ~ 55 1
8 3C 200 rG 08 27 25.38019 +29 18 44.9601   20       ~ 178 1
9 3C 207.0 Bla 08 40 47.58842599 +13 12 23.5637506   18.58 18.15 17.622   ~ 455 1
10 4C 58.17 Bla 08 54 41.99641612 +57 57 29.9391251   18.56 18.18 17.43   ~ 249 1
11 LB 9308 Sy1 09 06 31.8732919056 +16 46 11.785679112   18.48 18.27     ~ 303 3
12 4C 22.26 QSO 10 04 45.7421901264 +22 25 19.268460984   18.94 18.63     ~ 73 1
13 3C 243 QSO 10 26 31.9619676624 +06 27 33.028507440   19.00 18.62     ~ 122 1
14 4C 20.24 Bla 10 58 17.9007317832 +19 51 50.872721328   17.51 17.07 17.28   ~ 228 1
15 6C 111521+533608 QSO 11 18 12.2515418952 +53 19 43.945737420   19.19 18.73     ~ 39 1
16 7C 1218+3359 QSO 12 20 33.8756544048 +33 43 12.026168040   18.80 18.61     ~ 271 1
17 LBQS 1226+1035 QSO 12 28 36.8792519112 +10 18 41.954083020   19.33 19.12     ~ 102 1
18 ICRF J124357.6+162253 Sy1 12 43 57.6491122968 +16 22 53.395049244   19.23 19.00     ~ 321 1
19 4C 40.32 QSO 13 00 33.3077988648 +40 09 07.675089480   19.31 19.44     ~ 162 1
20 4C 11.45 QSO 13 21 18.8365075824 +11 06 49.991639544   19.55 19.32     ~ 122 2
21 4C 65.15 QSO 13 25 29.7054429984 +65 15 13.363097472   17.67 17.48     ~ 99 1
22 M 51 Sy2 13 29 52.698 +47 11 42.93   9.26 8.36 8.40   ~ 4565 4
23 4C 19.44 Bla 13 57 04.4366598768 +19 19 07.371837768   16.33 16.03 15.3   ~ 472 2
24 4C 11.50 Bla 15 50 43.5947388984 +11 20 47.453985024   17.47 17.23 16.5   ~ 175 3
25 2E 3648 Sy1 16 20 21.8185395384 +17 36 23.952361176   16.53 16.41 20.5   ~ 425 2
26 8C 1634+589 QSO 16 35 10.6394094312 +58 48 37.731273192   17.8 19.02 18.1   ~ 24 1
27 QSO B1634+176 QSO 16 36 16.7050693704 +17 35 07.870121700     18.0     ~ 53 1
28 4C 57.28 Bla 16 57 20.70895950 +57 05 53.5036669   18.59 18.28 17.4   ~ 76 1
29 3C 352 rG 17 10 44.1001 +46 01 29.834   22.8       ~ 150 1
30 4C 16.49 QSO 17 34 42.6025956120 +16 00 32.342065776     18.4     ~ 78 2
31 4C 47.48 QSO 18 18 19.5729871464 +47 36 43.897278600     18.2     ~ 43 1
32 4C 28.45 QSO 18 32 50.18562435 +28 33 35.9552173   16.91 17.16     ~ 137 1
33 4C 29.68 QSO 23 28 10.6609307784 +29 37 09.876341604   17.95 17.30     ~ 81 1
34 NAME Local Group GrG ~ ~           ~ 9325 0

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