2023MNRAS.526..750S


Query : 2023MNRAS.526..750S

2023MNRAS.526..750S - Mon. Not. R. Astron. Soc., 526, 750-757 (2023/November-3)

Search for particle acceleration in two massive Wolf-Rayet stars using uGMRT observations.

SAHA A., TEJ A., DEL PALACIO S., DE BECKER M., BENAGLIA P., ISHWARA-CHANDRA C.H. and PRAJAPATI P.

Abstract (from CDS):

Large wind kinetic power of Wolf-Rayet (WR) stars make them ideal targets in low radio frequencies to search for non-thermal emission due to relativistic particle acceleration. In this paper, we present observations of two WR stars, WR 114 and WR 142, in Band 4 (550-950 MHz) and Band 5 (1050-1450 MHz) using the upgraded Giant Meterwave Radio Telescope. Neither star is detected in the observed frequency bands, nor extended emission associated with them. The upper limit to the free-free radio emission from the stellar wind enables us to constrain the mass-loss rate of WR 114 to $\lesssim \rm 10^{-5}\, M_{ \odot }\, yr^{-1}$; this is a factor three smaller than previously estimated using spectroscopic modelling. If we further assume that the WR stars are binaries, the non-detection of synchrotron emission from the putative wind collision region implies that the stars are either in very wide binary systems away from periastron, or that the stars are in close binary systems with an orbital separation <70 AU for WR 114 and <20 AU for WR 142. The non-detection of low-frequency radio emission from these two systems thus provides evidence that narrows their nature, though it does not rule them out as bona fide particle-accelerating colliding-wind binaries.

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

Journal keyword(s): radiation mechanisms: non-thermal - radiation mechanisms: thermal - stars: Wolf-Rayet - radio continuum: ISM - stars: individual: WR 114 and WR 142

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 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
2 * gam02 Vel WR* 08 09 31.95013 -47 20 11.7108 0.64 1.58 1.83 1.85 2.00 WC8+O7.5III-V 951 0
3 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
4 V* V3893 Sgr WR* 17 45 47.5405102320 -26 10 26.779355616   15.13 14.20 14.23   WR 126 1
5 Ass Ser OB 1 As* 18 21 -14.4           ~ 76 0
6 PMN J1822-0939 Rad 18 22 28.792 -09 38 57.03           ~ 49 1
7 SNR G017.4-00.1 SNR 18 23.1 -13 46           ~ 23 0
8 HD 169010 WR* 18 23 16.3427231112 -13 43 26.102574732 13.53 12.99 12.02 11.95   WC 82 0
9 QSO B1908-202 Bla 19 11 09.65289294 -20 06 55.1090664   18.21   18.14   ~ 306 1
10 HD 190918 WR* 20 05 57.3244526328 +35 47 18.150756792 6.11 6.88 6.75     WN5+O9I 385 0
11 Ass Cyg OB 1 As* 20 17.8 +37 38           ~ 270 1
12 Cl Berkeley 87 OpC 20 21 35.0 +37 25 14           ~ 141 0
13 GAL 075.84+00.40 HII 20 21 38.3 +37 31 12           ~ 25 0
14 Onsala 2S HII 20 21 41.4 +37 25 44           ~ 41 0
15 GRS G075.78 +00.34 HII 20 21 43.6 +37 26 36           ~ 19 0
16 OH 075.8+00.3 HII 20 21 43.8 +37 26 39           ~ 95 2
17 WR 142 WR* 20 21 44.3438785440 +37 22 30.544989960   14.39 12.99 12.73 11.04 WO2 134 0
18 JCMTSF J202150.6+373010 HII 20 21 50.0 +37 30 15           ~ 12 0
19 BD+43 3654 s*b 20 33 36.0795027528 +43 59 07.364004504   11.24 10.06     O4If 76 0
20 MR 112 WR* 20 35 47.0859278605 +41 22 44.703520146     12.64 12.16   WC6+O8I-IIf 162 1
21 ICRF J205252.0+363535 Sy2 20 52 52.05501061 +36 35 35.3005698   22.083   21.200   ~ 112 2

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