Issue |
A&A
Volume 369, Number 1, April I 2001
|
|
---|---|---|
Page(s) | 142 - 154 | |
Section | Interstellar and circumstellar matter | |
DOI | https://doi.org/10.1051/0004-6361:20010095 | |
Published online | 15 April 2001 |
Bispectrum speckle interferometry observations and radiative transfer modelling of the red supergiant NML Cyg
Multiple dust-shell structures evidencing previous superwind phases
1
Max-Planck-Institut für Radioastronomie, Auf dem Hügel 69, 53121 Bonn, Germany e-mail: hofmann@mpifr-bonn.mpg.de; weigelt@mpifr-bonn.mpg.de
2
Special Astrophysical Observatory, Nizhnij Arkhyz, Zelenchuk region, Karachai-Cherkesia, 35147, Russia e-mail: balega@sao.ru
Corresponding author: T. Blöcker,bloecker@mpifr-bonn.mpg.de
Received:
16
November
2000
Accepted:
11
January
2001
NML Cyg is a highly evolved OH/IR supergiant,
one of the most prominent
infrared objects due to its strong obscuration by dust, and supposed to be
among the most luminous supergiants in the galaxy.
We present the first diffraction-limited
m observations of NML Cyg with
73 mas resolution. The speckle interferograms were obtained with the 6 m
telescope at the Special Astrophysical Observatory, and the
image reconstruction is based on the bispectrum speckle-interferometry method.
The visibility function declines towards the diffraction limit to ~0.6.
Radiative transfer calculations have been carried out to model the spectral
energy distribution, given by ground-based photo metry and ISO spectroscopy,
and our
m visibility function. Additionally,
mid-infrared visibility functions at
m were considered.
The observed dust shell properties do not appear to be in accordance with
standard single-shell (uniform outflow) models but seem to require
multiple components. Considering previous periods of
enhanced mass-loss, various density enhancements
in the dust shell were taken into account. An extensive grid of models was calculated for different
locations and strenghts of such superwind regions in the dust shell.
To match the observations from the optical to the
sub-mm domain requires at least two superwind regions embedded in the shell.
The best model includes a dust shell with a temperature of 1000 K at its
inner radius of
, a close embedded superwind shell extending
from
to
with an amplitude (factor of density enhancement) of 10,
and a far-out density enhancement at
with an amplitude of 5.
The angular diameters of the central star and of the inner rim
of the dust shell amount to 16.2 mas and 105 mas, resp.
The diameter of the embedded close superwind region extends from
263 mas to 368 mas, and the inner boundary of the distant superwind region
has a diameter of 3 fraction of arcsecond15.
In the near-infrared the dust condensation zone is limb-brightened leading
to a corresponding ring-like intensity distribution.
The grain sizes, a, were found to be in accordance with
a standard distribution function,
~ a-3.5, with a ranging between
m and
m.
The bolometric flux amounts to
Wm-2
corresponding to a central-star
luminosity of
.
Within the various parts of the dust shell,
density distributions
could be maintained differing only in their amplitude A.
A slight improvement of the far-infrared properties can be obtained if
a shallower density distribution of
is considered
in the distant superwind region.
The present-day mass-loss rate was determined to be
/yr.
The inner embedded superwind shell corresponds to a phase
of enhanced mass-loss (with amplitude 10)
in the immediate history of NML Cyg which began 59 yr ago and
lasted for ~18 yr.
Correspondingly, the outer superwind region is due to
to a high mass-loss period (amplitude 5) which terminated 529 yr ago.
Key words: techniques: image processing / circumstellar matter / stars: individual: NML Cyg / stars: mass / loss / stars: supergiants / infrared: stars
© ESO, 2001
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.