Astron. Astrophys. 322, 493-506 (1997)
1. Introduction
The study of pulsating stars is of great importance for the
construction of accurate stellar models, which provide in their turn
valuable clues to our understanding of stellar evolution. It has
indeed become clear that with detailed observational studies of the
pulsations one can probe the internal structure of the stars, and
hence confront the results with current theoretical stellar models
(see e.g. Winget et al. 1991, Matthews 1993, Breger 1995, Dziembowski
& Jerzykiewicz 1996).
The Cephei stars are one of the best studied
groups of early-type pulsating stars, in which both radial and
non-radial, and mono- and multiperiodic pulsations occur. Only
recently it was shown that the -mechanism
acting in a destabilising layer of the heavier elements is successful
in explaining the observed Cephei-type
pulsations (Cox & Morgan 1990, Dziembowski & Pamyatnykh 1993).
As the pulsation mechanism in these stars is still being tested
observationally, the detection and identification of pulsation modes
is of great importance for a confrontation with the recent theoretical
pulsation models.
The bright pulsating star Cep (HD205021,
spectral type B2III, V=3.2, 25 km/s) is the
prototype of this class of Cephei stars. The
radial-velocity variations of this star were first detected by Frost
(1902); the star is a radial pulsator with a period of 0.1905 days.
Since then, line-profile variations have been found which are periodic
at time scales of hours to decades.
Pigulski & Boratyn (1992) found that Cep
is the primary of a triple system; the secondary revolves around the
primary with an orbital period of 91.6 3.7
year. The secondary has been resolved by speckle interferometry
(Gezari et al. 1972), and the tertiary has a separation of 13.4
arcseconds (Heintz 1978).
A magnetic field strength of 810 170 G was
measured by Rudy & Kemp (1978). Henrichs et al. (1993) and Veen et
al. (1996) present measurements which emphasize the variable nature of
the magnetic field strength of Cep.
Besides the variable nature of the star itself,
Cep is also known to show variability of its
stellar wind (Fishel & Sparks 1972). Studies of the ultraviolet
(UV) wind lines of Cep (Fishel & Sparks
1981) revealed a 6 or 12 day period. Henrichs et al. (1993) and Veen
et al. (1996) identify the periodicity of the UV wind variability with
the rotation period of a magnetic dipole, which implies a rotation
period of the star of 12 days.
Long-term cycles of H absorption and
emission phases have been observed; the latest emission phase is
reported by Mathias et al. (1991) and Kaper & Mathias (1995).
Kaper et al. (1996) discuss whether the emission phases might be
associated with the binary nature, with a sudden change of the
amplitude of the radial pulsation, or with the magnetic activity of
the star.
Aerts et al. (1994) discovered short-term multi-periodicity in the
variations of optical lines of Cep. They
identified the frequency of the radial pulsation
=5.25 cycles/day, and found two more frequencies,
=5.38 c/d, =4.92 c/d,
close to the main frequency. The amplitude of these variations was
found to be much smaller than that of the radial pulsation. Aerts et
al. (1994) attributed these small variations at the newly found
frequencies to non-radial pulsation modes of the star, but labelled
the mode identifications as uncertain.
As a follow up on the work of Aerts et al. (1994), we investigate
if any possible effect of the presence of a magnetic field can be
found in the profile variations of the optical photospheric absorption
lines of the star. Furthermore, we investigate the characteristics of
the non-radial pulsation corresponding to the frequency
. Preliminary results of this work have been
presented by Telting et al. (1995).
The plan of our paper is as follows. A brief description of the
data is given in Sect. 2. In Sect. 3 we describe the period-search
methods that we have used to analyse the data, and list all the
frequencies that we find in the periodograms. The non-radial pulsation
in Cep is subject of the discussion in Sect. 4.
We discuss the observed frequency splitting in Sect. 5, and give some
concluding remarks in Sect. 6.
© European Southern Observatory (ESO) 1997
Online publication: June 5, 1998
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