2008A&A...484..801R


Query : 2008A&A...484..801R

2008A&A...484..801R - Astronomy and Astrophysics, volume 484, 801-813 (2008/6-4)

Multi-wavelength observations of Galactic hard X-ray sources discovered by INTEGRAL. II. The environment of the companion star.

RAHOUI F., CHATY S., LAGAGE P.-O. and PANTIN E.

Abstract (from CDS):

The INTEGRAL mission has led to the discovery of a new type of supergiant X-ray binaries (SGXBs), whose physical properties differ from those of previously known SGXBs. Those sources are in the course of being unveiled by means of multi-wavelength X-rays, optical, near- and mid-infrared observations, and two classes are appearing. The first class consists of obscured persistent SGXBs and the second is populated by the so-called supergiant fast X-ray transients (SFXTs). We report here mid-infrared (MIR) observations of the companion stars of twelve SGXBs from these two classes in order to assess the contribution of the star and the material enshrouding the system to the total emission. We used data from observations we carried out at ESO/VLT with VISIR, as well as archival and published data, to perform broad-band spectral energy distributions of the companion stars and fitted them with a combination of two black bodies representing the star and a MIR excess due to the absorbing material enshrouding the star, if there was any. We detect a MIR excess in the emission of IGR J16318-4848, IGR J16358-4726, and perhaps IGR J16195-4945. The other sources do not exhibit any MIR excess even when the intrinsic absorption is very high. Indeed, the stellar winds of supergiant stars are not suitable for dust production, and we show that this behaviour is not changed by the presence of the compact object. Concerning IGR J16318-4848 and probably IGR J16358-4726, the MIR excess can be explained by their sgB[e] nature and the presence of an equatorial disk around the supergiant companion in which dust can be produced. Moreover, our results suggest that some of the supergiant stars in those systems could exhibit an absorption excess compared to isolated supergiant stars, this excess being possibly partly due to the photoionisation of their stellar wind in the vicinity of their atmosphere. We also show that the differences in behaviour between the obscured SGXBs and the SFXTs in the high-energy domain do not exist from optical-to-MIR wavelength. Supergiant stars in SFXTs could nevertheless be most of the time less absorbed than supergiant stars in obscured SGXBs, due to the geometry of the systems. At last, our results confirm a very dense cocoon of material around the compact object as the extinction in the X-ray domain is generally several orders of magnitude higher than the extinction in the visible.

Abstract Copyright:

Journal keyword(s): stars: fundamental parameters - infrared: stars - X-rays: binaries - stars: binaries: general - stars: supergiants

CDS comments: Paragraph 3.4 2MASS J16320215-4752289 is a probable misprint for 2MASS J16320215-4752322. Paragraph 4.4 IGR J16465-4945 is a misprint for IGR J16465-4507 or for IGR J16195-4945.

Simbad objects: 29

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Number of rows : 29
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 HD 144969 s*b 16 10 49.1477658960 -48 47 41.747601948 9.14 9.32 8.39 7.47 6.70 B1Ia 69 0
2 SSTGLMC G333.4590+01.0501 MIR 16 16 02.880 -49 18 02.10           ~ 1 0
3 HD 146628 * 16 19 29.5214538960 -49 45 40.715149896 10.23 10.58 10.06 10.02   B1/2Ia 70 1
4 IGR J16195-4945 HXB 16 19 32.1832111152 -49 44 30.565493340   17.4 16.8 15.3 15.295 ON9.7Iab 54 0
5 IGR J16207-5129 HXB 16 20 46.2644580432 -51 30 06.045320232   18.9   16.28 13.4 B1Ia 62 0
6 HD 148422 * 16 30 59.8917961848 -56 29 43.228963104 7.93 8.70 8.65 9.40   B1Ia 75 0
7 IGR J16318-4848 HXB 16 31 48.3090342864 -48 49 00.665054832         16.217 B[e]I 173 0
8 SSTGLMC G335.6260-00.4477 MIR 16 31 50.800 -48 48 34.36           ~ 1 0
9 IGR J16320-4751 HXB 16 32 01.76 -47 52 29.0           BN0.5Ia 175 0
10 2MASS J16320215-4752322 * 16 32 02.1634603488 -47 52 32.294654472   17.3 16.1     K 7 1
11 * mu. Nor s*b 16 34 05.0193637737 -44 02 43.120603946 4.05 4.99 4.94 6.36   O9.7Iab 275 0
12 2MASS J16355369-4725398 NIR 16 35 53.70 -47 25 39.8           ~ 9 1
13 SSTGLMC G337.0994-00.0062 MIR 16 35 53.740 -47 25 40.03           ~ 1 0
14 [KRL2007b] 194 Psr 16 36 30 -47 37.5           Be 86 0
15 IGR J16418-4532 HXB 16 41 50.7984926736 -45 32 25.366995132           BN0.5Ia 109 0
16 IGR J16465-4507 HXB 16 46 35.2590465192 -45 07 04.609890912       14.033   O9.5Ia 98 0
17 IGR J16479-4514 HXB 16 48 06.56184 -45 12 06.8148           O9.5Iab 134 0
18 DENIS J164806.8-451207 * 16 48 06.8538293712 -45 12 07.979112072         17.802 ~ 4 0
19 HD 151804 s*b 16 51 33.7218052272 -41 13 49.919519496 4.45 5.29 5.22     O8Iaf 376 0
20 HD 152235 s*b 16 53 58.8528412848 -41 59 39.577848180 6.47 6.92 6.38 5.84 5.42 B0.5Ia 192 0
21 HD 152234 s*b 16 54 01.8373779952 -41 48 22.987396952 4.92 5.64 5.45     B0.5Ia 194 0
22 HD 152249 s*b 16 54 11.6395658856 -41 50 57.295111524 5.91 6.65 6.45     OC9Iab 239 0
23 HD 153919 HXB 17 03 56.7725629224 -37 50 38.913331452 6.06 6.78 6.51 6.08 5.90 O6Iafcp 814 1
24 HD 156201 * 17 17 45.5144080704 -35 13 27.017180436 8.34 8.70 8.01 7.31   B0.5Ia/ab 62 0
25 2MASS J17251139-3616575 HXB 17 25 11.392 -36 16 57.53     14.30     B0-1Ia 126 2
26 AX J1739.1-3020 HXB 17 39 11.5515537336 -30 20 37.787917704     14.40 13.91   O8.5Iab(f) 157 1
27 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 14421 0
28 IGR J17544-2619 HXB 17 54 25.2722906112 -26 19 52.576928292   14.71 12.94 12.10 10.38 O9Ib 190 0
29 IGR J19140+0951 HXB 19 14 04.2271468632 +09 52 58.399995144   18.6 16.4     B1Iab 104 0

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