2023MNRAS.523..701W


Query : 2023MNRAS.523..701W

2023MNRAS.523..701W - Mon. Not. R. Astron. Soc., 523, 701-719 (2023/July-3)

A morphological analysis of the substructures in radio relics.

WITTOR D., BRUGGEN M., GRETE P. and RAJPUROHIT K.

Abstract (from CDS):

Recent observations of radio relics - diffuse radio emission in galaxy clusters - have revealed that these sources are not smooth but consist of structures in the form of threads and filaments. We investigate the origin of these filamentary structures and the role of projection effects. To this end, we have developed a tool that extracts the filamentary structures from background emission. Moreover, it is capable of studying both two-dimensional and three-dimensional objects. We apply our structure extractor to both observations and cosmological simulations of radio relics. Using Minkowski functionals, we determine the shape of the identified structures. In our 2D analysis, we find that the brightest structures in the observed and simulated maps are filaments. Our analysis of the 3D simulation data shows that radio relics do not consist of sheets but only of filaments and ribbons. Furthermore, we did not find any measurable projection effect that could hide any sheet-like structures in projection. We find that both the magnetic field and the shock front consist of filaments and ribbons that cause filamentary radio emission.

Abstract Copyright: © 2023 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): magnetic fields - shock waves - techniques: image processing - software: data analysis - galaxies: clusters: intracluster medium - radio continuum: general

Simbad objects: 4

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Number of rows : 4
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 2744 ClG 00 14 20.03 -30 23 17.8           ~ 1077 0
2 ACO 3376 ClG 06 01 25.000 -39 59 51.00           ~ 334 0
3 ACO 2256 ClG 17 03 37.5 +78 37 23           ~ 928 1
4 ACO 3667 ClG 20 12 33.68 -56 50 26.3           ~ 676 1

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