Bibcode
DOI
Lobel, A.; Dupree, A. K.; Stefanik, R. P.; Torres, G.; Israelian, G.; Morrison, N.; de Jager, C.; Nieuwenhuijzen, H.; Ilyin, I.; Musaev, F.
Referencia bibliográfica
The Astrophysical Journal, Volume 583, Issue 2, pp. 923-954.
Fecha de publicación:
2
2003
Revista
Número de citas
86
Número de citas referidas
67
Descripción
We present an overview of the spectral variability of the peculiar
F-type hypergiant ρ Cas, obtained from our long-term monitoring
campaigns over the past 8.5 yr with four spectrographs in the northern
hemisphere. Between 2000 June and September an exceptional variability
phase occurred when the V brightness dimmed by about a full magnitude.
The star recovered from this deep minimum by 2001 April. It is the third
outburst of ρ Cas on record in the last century. We observe TiO
absorption bands in high-resolution near-IR spectra obtained with the
Utrecht Echelle Spectrograph during the summer of 2000. TiO formation in
the outer atmosphere occurred before the deep brightness minimum.
Atmospheric models reveal that the effective temperature decreases by at
least 3000 K, and the TiO shell is driven supersonically with
M~=5.4×10-2 Msolar yr-1. Strong
episodic mass loss and TiO have also been observed during the outbursts
of 1945-1947 and 1985-1986. A detailed analysis of the exceptional
outburst spectra is provided, by comparing with high-resolution optical
spectra of the early M-type supergiants μ Cep (Ia) and Betelgeuse
(Iab). During the outburst, central emission appears above the local
continuum level in the split Na D lines. A prominent optical emission
line spectrum appears in variability phases of fast wind expansion. The
radial velocity curves of Hα and of photospheric metal absorption
lines signal a very extended and velocity-stratified dynamic atmosphere.
The outburst spectra indicate the formation of a low-temperature,
optically thick circumstellar gas shell of 3×10-2
Msolar during 200 days, caused by dynamic instability of the
upper atmosphere of this pulsating massive supergiant near the Eddington
luminosity limit. We observe that the mass-loss rate during the outburst
is of the same order of magnitude as has been proposed for the outbursts
of η Carinae. We present calculations that correctly predict the
outburst timescale, whereby the shell ejection is driven by the release
of hydrogen ionization recombination energy.