2025PASJ...77..480Z


Query : 2025PASJ...77..480Z

2025PASJ...77..480Z - Publ. Astron. Soc. Jap., 77, 480-487 (2025/June-0)

An XMM-Newton study of Kesteven 69: Challenging the classification as a typical thermal composite supernova remnant?

ZHANG K.

Abstract (from CDS):

Supernova remnants are diffuse nebulae generated by the interaction of supernova explosions with the surrounding environment, usually observed in the X-ray band. Thermal composite supernova remnants are primarily characterized by their center-brightened emission, yet they lack an associated pulsar wind nebula. Within this category, Kesteven 69 has traditionally been the sole candidate without gamma-ray detection or recombining plasma emission. In this study, the first Australian Square Kilometre Array Pathfinder image and the XMM-Newton background-subtracted image are presented, and spatially resolved spectral analyses are described. These multiwavelength investigations reveal a novel perspective that Kesteven 69 is likely to be a shell-type supernova remnant located on the periphery of molecular clouds, featuring two major X-ray arcs. This finding suggests a reevaluation of the unusual morphology observed in other special thermal composite supernova remnant candidates.

Abstract Copyright: © The Author(s) 2025. Published by Oxford University Press on behalf of the Astronomical Society of Japan.

Journal keyword(s): ISM: individual objects (G21.8-0.6, Kesteven 69) - ISM: supernova remnants - X-rays: ISM

Simbad objects: 7

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Number of rows : 7
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 SNR G327.4+00.4 SNR 15 48 20 -53 49.0           ~ 97 0
2 NAME LHB X 16 42.0 +02 19           ~ 414 0
3 SNR G352.7-00.1 SNR 17 27 43 -35 06.5           ~ 79 1
4 [ABB2014] WISE G021.884-00.318 IR 18 32 12 -09 57.8           ~ 2 0
5 SNR G021.8-00.6 SNR 18 32 45 -10 08.0           ~ 137 0
6 NAME Cyg Loop SNR 20 51.0 +30 40           ~ 964 0
7 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1

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