2003A&A...408..715B


Query : 2003A&A...408..715B

2003A&A...408..715B - Astronomy and Astrophysics, volume 408, 715-727 (2003/9-3)

Radio and submillimetre observations of wind structure in ζ Puppis.

BLOMME R., VAN DE STEENE G.C., PRINJA R.K., RUNACRES M.C. and CLARK J.S.

Abstract (from CDS):

We present radio and submillimetre observations of the O4I(n)f star ζ Pup, and discuss structure in the outer region of its wind (∼10-100R*). The properties of bremsstrahlung, the dominant emission process at these wavelengths, make it sensitive to structure and allow us to study how the amount of structure changes in the wind by comparing the fluxes at different wavelengths. Possible forms of structure at these distances include Corotating Interaction Regions (CIRs), stochastic clumping, a disk or a polar enhancement. As the CIRs are azimuthally asymmetric, they should result in variability at submillimetre or radio wavelengths. To look for this variability, we acquired 3.6 and 6-cm observations with the Australia Telescope Compact Array (ATCA), covering about two rotational periods of the star. We supplemented these with archive observations from the NRAO Very Large Array (VLA), which cover a much longer time scale. We did not find variability at more than the ±20% level. The long integration time does allow an accurate determination of the fluxes at 3.6 and 6-cm. Converting these fluxes into a mass loss rate, we find {dot}(M)=3.5x10–6M/yr. This value confirms the significant discrepancy with the mass loss rate derived from the Hα profile, making ζ Pup an exception to the usually good agreement between the Hα and radio mass loss rates. To study the run of structure as a function of distance, we supplemented the ATCA data by observing ζ Pup at 850µm with the James Clerk Maxwell Telescope (JCMT) and at 20-cm with the VLA. A smooth wind model shows that the millimetre fluxes are too high compared to the radio fluxes. While recombination of helium in the outer wind cannot be discounted as an explanation, the wealth of evidence for structure strongly suggests this as the explanation for the discrepancy. Model calculations show that the structure needs to be present in the inner ∼70R* of the wind, but that it decays significantly, or maybe even disappears, beyond that radius.

Abstract Copyright:

Journal keyword(s): stars: early-type - stars: individual: ζ Pup - stars: mass loss - stars: winds, outflows - radio continuum: stars

Nomenclature: Table 4: [BVP2003] SN (Nos S2-S7).

Simbad objects: 17

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Number of rows : 17
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 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2812 2
2 V* HL Tau Or* 04 31 38.5107609312 +18 13 57.859747968   15.89 14.49 14.39   K5 1423 0
3 IRAS 04287+1807 mul 04 31 38.8 +18 13 57           ~ 796 0
4 * eps Ori s*b 05 36 12.81335 -01 12 06.9089 0.48 1.51 1.69 1.76 1.93 B0Ia 896 0
5 QSO J0730-116 QSO 07 30 19.11247452 -11 41 12.6006642     20.30 20.3   ~ 300 1
6 NVSS J080310-395729 Rad 08 03 10.87 -39 57 29.8           ~ 1 0
7 NVSS J080321-400153 Rad 08 03 21.54 -40 01 56.9           ~ 1 0
8 [BVP2003] S4 Rad 08 03 24.38 -39 59 49.2           ~ 1 0
9 NVSS J080327-395828 Rad 08 03 28.65 -39 58 20.4           ~ 1 0
10 * 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
11 [BVP2003] S7 Rad 08 03 44.03 -39 57 56.5           ~ 1 0
12 PMN J0814-3539 Rad 08 14 14.64 -35 38 25.7           ~ 3 1
13 ICRF J082526.8-501038 QSO 08 25 26.8673494560 -50 10 38.484054768   20.94       ~ 133 1
14 QSO B0826-373 QSO 08 28 04.78023133 -37 31 06.2815112   16       ~ 57 0
15 QSO B0834-201 QSO 08 36 39.21525204 -20 16 59.5042773   19.45 19.4 18.76   ~ 209 1
16 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4338 2
17 ICRF J193925.0-634245 Sy2 19 39 25.0245304992 -63 42 45.640373400   18.87 18.37 17.64   ~ 1224 1

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