High-resolution, high signal-to-noise spectroscopic observations have shown
that the presence of multiperiodic variability in photospheric lines is
rather common among hot stars of luminosity class V-III (Kambe et al. 1990;
Floquet et al. 1992, 1996; Gies & Kullavanijaya 1988). Spectroscopic observations of
rapid rotators (e.g., Be stars) with sufficient temporal resolution have shown
that the observed line profile variability (lpv) is characterized by the
presence of "moving bumps" travelling from blue to red across the line profile
in timescales of hours. The prototype object showing this kind of
behavior is the Be star
Ophiuchi. The phenomenon has also been observed
in O stars and
Scuti variables (Kennelly et al. 1992, hereafter KWM)
among others. Non-radial pulsations (NRP) have been proposed as an explanation
for the lpv observed in hot stars (e.g., Smith 1977; Gies 1991 and
references therein). NRP produce lpv thanks to the combination of the
Doppler displacement of stellar surface elements with their associated
temperature variations due to the compression/expansion caused by the passage
of the waves through the photosphere. In favorable cases these variations can
also be detected photometrically. In rapid rotators, there is a one-to-one
correlation between the points in the broaded line profile and the position of
inhomogeneities on the stellar surface (the so-called "Doppler Imaging"). The
additional velocity fields due to NRP produce then series of "bumps" that will
move from blue to red across the line profile due to the stellar rotation and wave motion (Vogt &
Penrod 1983).
Be stars are rapid rotators of spectral type late O to
early A and luminosity class V-III, showing a near infrared excess and Balmer
emission lines imputed to an equatorially concentrated circumstellar envelope,
produced by sporadic mass ejection episodes. The causes of the "abnormal" mass
loss are as yet unknown. In spite of their high , rapid rotation
alone cannot explain ejection episodes as Be stars are not observed to rotate
sufficiently near the break-up velocity. NRP could be the clue to the Be
phenomenon, providing the surplus of perturbation that is needed to cause mass
ejection. Thanks to recent theoretical models that explain the
excitation of NRP in hot stars through opacity mechanisms (Dziembowski &
Pamyatnykh 1991, 1993; Gautschy & Saio 1993), the idea that lpv in B-Be
stars can be caused by NRP has been reinforced. In fact, the presence of NRP in
B-Be stars (the so-called "Slowly-Pulsating Variables" - SPB) is a logical issue
in the sense that it bridges the gap along the main sequence between
Cephei
and
Scuti pulsating variables (Dziembowski 1997). In this
paper, we present the results of an extensive search for periodic oscillations
in the
Oph-type Be star
Cen. The observational material
consists of spectroscopic and photometric observations conducted at
Laboratório Nacional de Astrofísica (LNA) (Pico dos Dias, MG-Brazil).
Frequency analysis has been performed by means of algorithms
employing Fourier techniques. Photometric and spectroscopic data of
Cuypers et al. (1989) and Stefl et
al. (1995, hereafter SBHB) and photometric observations obtained with the
Hipparcos satellite are also reconsidered.
Cen (HD 127972; HR 5440; SAO 225044; MWC
232) is a rapidly-rotating (
km s-1), bright (V
2.3) early-type Be/shell star. Cuypers et al. (1989) and Cuypers (1991)
found triple-wave and double-wave photometric
modulations with periods 1.92 d and 1.28 d, respectively. Bumps moving
across the HeI 667.8 nm profile detected by Leister et al. (1994) were
attributed to a NRP mode with
m
=l
15 or
m
6, l
7.
Variability in both lpv (visible) and UV flux with a timescale of
1.64 c/d was detected by Gies (1994). Stefl et al. (1995)
found nearly sinusoidal brightness (Strömgren system) and radial velocity
variations (SiIII
455.26 nm line) with period p=0.64 d (1.56 c/d).
Finally, the Hipparcos catalogue (ESA 1997) quotes for the star a photometric
period of 1.28 d (
0.78 c/d).
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