2024A&A...691A.132R


Query : 2024A&A...691A.132R

2024A&A...691A.132R - Astronomy and Astrophysics, volume 691A132 (2024/11-1)

Cosmic evolution of the Faraday rotation measure in the intracluster medium of galaxy clusters.

RAPPAZ Y., SCHOBER J., BENDRE A.B., SETA A. and FEDERRATH C.

Abstract (from CDS):

Context. Radio observations have revealed magnetic fields in the intracluster medium (ICM) of galaxy clusters, and their energy density is nearly in equipartition with the turbulent kinetic energy. This suggests magnetic field amplification by dynamo processes during cluster formation. However, observations are limited to redshifts ɀ ≲ 0.7, and the weakly collisional nature of the ICM complicates studying magnetic field evolution at higher redshifts through theoretical models and simulations.
Aims. Using a model of the weakly collisional dynamo, we modelled the evolution of the Faraday rotation measure (RM) in galaxy clusters of different masses, up to ɀ ≃ 1.5, and investigated its properties such as its radial distribution up to the virial radius r200. We compared our results with radio observations of various galaxy clusters.
Methods. We used merger trees generated by the modified GALFORM algorithm to track the evolution of plasma quantities during galaxy cluster formation. Assuming the magnetic field remains in equipartition with the turbulent velocity field, we generated RM maps to study their properties.
Results. We find that both the standard deviation of RM, σRM, and the absolute average |µRM| increase with cluster mass. Due to redshift dilution, RM values for a fixed cluster mass remain nearly constant between ɀ = 0 and ɀ = 1.5. For r/r200 ≳ 0.4, σRM does not vary significantly with ℒ/r200, with ℒ being the size of the observed RM patch. Below this limit, σRM increases as ℒ decreases. We find that radial RM profiles have a consistent shape, proportional to 10^-1.2(r/r200)^, and are nearly independent of redshift. Our ɀ ≃ 0 profiles for Mclust = 1015 M⊙ match RM observations in the Coma cluster but show discrepancies with Perseus, possibly due to high gas mixing. Models for clusters with Mclust = 1013 and 1015 M⊙ at ɀ = 0 and ɀ = 0.174 align well with Fornax and A2345 data for r/r200 ≲ 0.4. Our model can be useful for generating mock polarization observations for current and next-generation radio telescopes.

Abstract Copyright: © The Authors 2024

Journal keyword(s): dynamo - magnetic fields - magnetohydrodynamics (MHD) - plasmas - turbulence - large-scale structure of Univers

Simbad objects: 21

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Number of rows : 21
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 ACO 119 ClG 00 56 08.57 -01 12 00.8           ~ 577 2
2 ACO 225 ClG 01 38 55 +18 53.2           ~ 54 0
3 ACO 376 ClG 02 45 48 +36 51.6           B8.5 161 1
4 ACO 400 ClG 02 57 37.4 +06 00 45           ~ 408 3
5 ACO 426 ClG 03 19 47.6 +41 30 54           ~ 2508 1
6 NGC 1316 rG 03 22 41.789 -37 12 29.52 9.81 9.15 8.53 7.66   ~ 1491 1
7 NGC 1399 rG 03 38 29.083 -35 27 02.67 11.05 9.74 9.59 8.12   ~ 1636 1
8 ACO S 373 ClG 03 38 29.4 -35 27 08           ~ 2029 0
9 ACO 496 ClG 04 33 40.8 -13 14 34           ~ 728 2
10 ACO 514 ClG 04 48 18 -20 28.7           ~ 149 0
11 NAME HYA SUPERCL SCG 08 57.9 +03 10           ~ 204 0
12 ACO 754 ClG 09 09 14.8 -09 40 35           ~ 695 1
13 ACO 780 ClG 09 18 30 -12 15.7           ~ 469 0
14 NAME Hydra I Cluster ClG 10 36 36.0 -27 31 04           ~ 905 1
15 ACO 1314 ClG 11 34 53.0 +49 05 18           ~ 234 1
16 NAME NGC 4839 Group GrG 12 57 21.5 +27 31 54           ~ 86 0
17 ACO 1656 ClG 12 59 44.40 +27 54 44.9           ~ 5141 2
18 ACO 2247 ClG 16 47 22 +81 34.0           ~ 59 0
19 ACO 2255 ClG 17 12 56.0 +64 04 06           ~ 605 0
20 ACO 2345 ClG 21 27 05.391 -12 09 07.41           ~ 151 0
21 ACO 2634 ClG 23 38 18.4 +27 01 37           ~ 515 2

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