2014ApJ...789..163L


Query : 2014ApJ...789..163L

2014ApJ...789..163L - Astrophys. J., 789, 163 (2014/July-2)

Diagnostics of the solar Corona from comparison between Faraday rotation measurements and magnetohydrodynamic simulations.

LE CHAT G., KASPER J.C., COHEN O. and SPANGLER S.R.

Abstract (from CDS):

Polarized natural radio sources passing behind the Sun experience Faraday rotation as a consequence of the electron density and magnetic field strength in coronal plasma. Since Faraday rotation is proportional to the product of the density and the component of the magnetic field along the line of sight of the observer, a model is required to interpret the observations and infer coronal structures. Faraday rotation observations have been compared with relatively ad hoc models of the corona. Here for the first time we compare these observations with magnetohydrodynamic (MHD) models of the solar corona driven by measurements of the photospheric magnetic field. We use observations made with the NRAO Very Large Array of 34 polarized radio sources occulted by the solar corona between 5 and 14 solar radii. The measurements were made during 1997 May, and 2005 March and April. We compare the observed Faraday rotation values with values extracted from MHD steady-state simulations of the solar corona. We find that (1) using a synoptic map of the solar magnetic field just one Carrington rotation off produces poorer agreements, meaning that the outer corona changes in the course of one month, even in solar minimum; (2) global MHD models of the solar corona driven by photospheric magnetic field measurements are generally able to reproduce Faraday rotation observations; and (3) some sources show significant disagreement between the model and the observations, which appears to be a function of the proximity of the line of sight to the large-scale heliospheric current sheet.

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Journal keyword(s): magnetohydrodynamics, MHD - methods: numerical - Sun: corona - Sun: magnetic fields

Simbad objects: 29

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Number of rows : 29
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 4C -00.01 QSO 00 06 22.6058589240 -00 04 24.453903468   20.14 19.35     ~ 196 1
2 4C 04.01 Rad 00 23 19.993 +04 28 56.13           ~ 4 1
3 [VV98] J002903.5+050934 Bla 00 29 03.5918457912 +05 09 34.864702740   20.0 19.0 18.6   ~ 51 1
4 4C 05.05 rG 00 30 40.80984 +05 47 16.3392           ~ 5 1
5 4C 00.04 QSO 00 34 19.1744629656 +01 18 36.194716440     18.56     ~ 21 1
6 NGC 193 rG 00 39 18.5878961880 +03 19 52.605787764   14.3       ~ 149 1
7 4C 06.03 Rad 00 41 32.428 +06 57 53.42           ~ 6 1
8 4C 05.06 Rad 00 46 44.003 +06 10 02.74           ~ 4 1
9 4C 15.09 QSO 02 51 46.8035292048 +15 50 13.191691992     19.0     ~ 25 1
10 3C 74 Rad 02 53 59.077 +20 14 56.19           ~ 25 2
11 3C 76.1 rG 03 03 15.0210658512 +16 26 18.881230884   16.00 14.86     ~ 182 2
12 3C 79.0 Sy2 03 10 00.0936589848 +17 05 58.599361932   19.54 18.75     ~ 268 3
13 PKS 0319+176 Rad 03 22 22.4 +17 48 08           ~ 3 0
14 4C 22.06 Rad 03 52 33.376 +22 20 19.74           ~ 10 1
15 4C 18.11 QSO 03 56 33.4732368024 +19 00 35.005035780     19.0     ~ 17 2
16 PKS 0403+208 rG 04 06 21.5957433696 +20 56 23.464748688           ~ 15 0
17 3C 108 QSO 04 12 43.66686922 +23 05 05.4525810   19.60 18.70     ~ 100 1
18 3C 114 rG 04 20 22.104 +17 53 54.82   22       ~ 72 2
19 QSO B2320-035 Bla 23 23 31.95375055 -03 17 05.0238540   18.6   18.16   ~ 229 2
20 4C -05.96 rG 23 25 19.581 -04 57 36.70     18.5     ~ 23 1
21 ICRF J232653.7-020213 BLL 23 26 53.77670595 -02 02 13.7811657   18.3       ~ 60 1
22 4C -05.97 Rad 23 28 12.073 -04 56 09.40           ~ 9 1
23 PMN J2331-0129 rG 23 31 13.540 -01 29 11.09           ~ 6 1
24 QSO B2332-017 Bla 23 35 20.41204300 -01 31 09.5917037   18.4 18.78 18.35   ~ 116 1
25 QSO B2335-027 Bla 23 37 57.33907021 -02 30 57.6293054   18.1 19.27 18.97   ~ 146 1
26 4C -04.89 Rad 23 38 59.152 -04 13 37.66           ~ 12 1
27 4C -01.61 BLL 23 51 56.1224889360 -01 09 13.315371768   16.83 16.59     ~ 380 1
28 PKS 2350-018 Rad 23 52 50.152 -01 36 10.73     19.5     ~ 7 1
29 4C -02.91 Rad 23 57 05.69 -02 26 38.4           ~ 16 1

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