2025A&A...694A.125L


Query : 2025A&A...694A.125L

2025A&A...694A.125L - Astronomy and Astrophysics, volume 694A125 (2025/2-1)

The MeerKAT Fornax Survey IV. A close look at the cluster physics through the densest rotation measure grid.

LOI F., SERRA P., MURGIA M., GOVONI F., VACCA V., MACCAGNI F., KLEINER D. and KAMPHUIS P.

Abstract (from CDS):

Using the Square Kilometre Array (SKA) mid precursor MeerKAT, we acquired broadband spectro-polarimetric data in the context of the MeerKAT Fornax Survey to study the Fornax cluster's magnetic fields in detail by building the densest rotation measure (RM) grid to date. Here, we present the survey, the analysis, and a discussion of the RM grid properties. We analyzed a circular region centered on the Fornax cluster center with a radius of ∼1.4°; that is, ∼0.73Rvir. The mosaics have a resolution of 13″ and cover the frequencies between 900 MHz and 1.4 GHz, reaching an average noise of 16 μJy beam–1 in total intensity and 3 μJy beam–1 in the Q and U Stokes images. With these data, we detected 508 polarized sources over an area of ∼6.35 deg2 corresponding to a density of ∼80 polarized sources/deg2. This is the densest RM grid ever built. Of the polarized sources, five are cluster sources. Excluding the cluster sources, we built the Euclidean-normalized differential source counts in polarization and we went a factor of ten deeper than previous surveys. We tentatively detect for the first time an increment in the differential source counts at low polarized flux densities; that is, ∼9 μJy at 1.4 GHz. The average degree of polarization of about 3-4% suggests that the sub-μJansky population is not dominated by star-forming galaxies, typically showing a degree of polarization lower than 1%. The majority of the polarized sources are Faraday simple; in other words, their polarization plane rotates linearly with the wavelength squared. The RM shows the typical decrement going from the center to the outskirts of the Fornax cluster. However, interesting features are observed both in the RM grid and in the RM radial profiles across different directions. A combination of the cluster physics and large-scale structure filaments surrounding the Fornax cluster could explain the RM characteristics.

Abstract Copyright: © The Authors 2025

Journal keyword(s): magnetic fields - polarization - surveys - galaxies: clusters: individual: Fornax cluster

Simbad objects: 15

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Number of rows : 15
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 ELAIS S1 reg 00 34 44 -43 28.2           ~ 254 0
2 NAME XMM-LSS Field reg 02 18 00 -07 00.0           ~ 347 0
3 NAME Chandra Deep Field-South reg 03 32 28.0 -27 48 30           ~ 2282 1
4 NGC 1365 Sy1 03 33 36.458 -36 08 26.37 10.48 10.08 9.63 8.79 9.7 ~ 1987 2
5 NGC 1380 Sy2 03 36 27.590 -34 58 34.68 11.32 10.94 9.93 9.37   ~ 460 1
6 NGC 1386 Sy1 03 36 46.238 -35 59 57.39 12.42 12.16 11.23 10.76   ~ 553 1
7 NGC 1387 Sy2 03 36 57.0337458600 -35 30 23.675934060 12.18 11.75 10.69 10.16   ~ 290 1
8 NGC 1399 rG 03 38 29.083 -35 27 02.67 11.05 9.74 9.59 8.12   ~ 1636 1
9 ACO S 373 ClG 03 38 29.4 -35 27 08           ~ 2029 0
10 NAME Eridanus ClG GrG 03 38 32.00 -22 18 51.0           ~ 200 0
11 NAME NGC 1566 Group GrG 04 20 00.6 -54 56 17           ~ 180 0
12 ICRF J052109.8+163822 Sy1 05 21 09.88596258 +16 38 22.0515459   19.37 18.84 18.480   ~ 910 1
13 NAME COSMOS Field reg 10 00 28.60 +02 12 21.0           ~ 3639 0
14 NAME Lockman Hole reg 10 45 00.0 +58 00 00           ~ 910 0
15 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2

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