2012MNRAS.422.1332Z


Query : 2012MNRAS.422.1332Z

2012MNRAS.422.1332Z - Mon. Not. R. Astron. Soc., 422, 1332-1342 (2012/May-2)

X-rays from colliding stellar winds: the case of close Wolf-Rayet+O binary systems.

ZHEKOV S.A.

Abstract (from CDS):

We have analysed the X-ray emission from a sample of close Wolf-Rayet+O (WR+O) binaries using data from the public Chandra and XMM-Newton archives. Global spectral fits show that two-temperature plasma is needed to match the X-ray emission from these objects, because the hot component (kT > 2 keV) is an important ingredient of the spectral models. In close WR+O binaries, X-rays likely originate in colliding stellar wind (CSW) shocks, driven by the massive winds of the binary components. The CSW shocks in these objects are expected to be radiative because of the high density of the plasma in the interaction region. In contrast, our analysis shows that, in our sample of close WR+O binaries, the CSW shocks are adiabatic. This is possible only if the mass-loss rates of the stellar components in the binary are at least one order of magnitude smaller than the values currently accepted. The most likely explanation for the X-ray properties of close WR+O binaries is that their winds are two-component flows. The more massive component (dense clumps) has a role in the optical/ultraviolet emission from these objects, while the smooth rarefied component is a key factor in the X-ray emission from these objects.

Abstract Copyright: 2012 The Author Monthly Notices of the Royal Astronomical Society2012 RAS

Journal keyword(s): shock waves - stars: Wolf-Rayet - X-rays: binaries - X-rays: stars

Nomenclature: Fig. A2: [Z2012] SN (Nos S1-S2).

Simbad objects: 18

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Number of rows : 18
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 * zet Pup BY* 08 03 35.04754 -40 00 11.3321 0.89 1.98 2.25 2.36 2.58 O4I(n)fp 1154 1
2 Cl* NGC 3603 BLW A1 WR* 11 15 07.31 -61 15 38.4   12.32 11.18     WN6h 70 0
3 NGC 3603 OpC 11 15 10.8 -61 15 32           ~ 1065 1
4 HD 104994 WR* 12 05 18.7204232424 -62 03 10.140656832 9.95 10.94 10.93 11.03   WN3p-w 166 0
5 HD 311884 WR* 12 43 50.9991209208 -63 05 14.812489320 11.45 11.64 10.81 10.59   WN6+O5V 170 0
6 * tet Mus WR* 13 08 07.1531705448 -65 18 21.679426548 4.71 5.50 5.53 5.44 5.40 WC5+B0III 318 0
7 CXOU J165419.3-414908 Y*? 16 54 19.3964977776 -41 49 08.397706368           ~ 3 0
8 CXOU J165419.4-414916 Y*? 16 54 19.429 -41 49 16.74           ~ 3 0
9 HD 152270 WR* 16 54 19.6991292072 -41 49 11.531710092 6.26 6.80 6.597 6.72 6.39 WC7+O5-8 303 0
10 HD 159176 Be* 17 34 42.4921337376 -32 34 53.995451196 4.88 5.74 5.70 7.19   O7V 254 0
11 NAME Sgr A* X 17 45 40.03599 -29 00 28.1699           ~ 4388 3
12 GCIRS 16S WR* 17 45 40.09 -29 00 29.8           ~ 12 0
13 HD 193576 WR* 20 19 32.4229160448 +38 43 53.959035756 8.15 8.53 8.00     WN5+O6II-V 707 0
14 HD 193793 WR* 20 20 27.9757908696 +43 51 16.286840244 6.90 7.25 6.85 4.58   WC7pd+O5.5fc 710 0
15 HD 193928 WR* 20 21 31.7290073688 +36 55 12.773070696 10.67 10.60 9.78     WN5-w+O5V-III 199 0
16 EM* AS 422 WR* 20 32 06.2786571432 +40 48 29.527101576   13.46 11.83     WN7o/CE+O7V(f) 101 0
17 Ass Cyg OB 2 As* 20 33.2 +41 19           ~ 943 0
18 HD 197406 WR* 20 41 21.5485520640 +52 35 15.142636896 10.42 10.87 10.30     WN8h+B3IV/BH 197 0

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