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Astron. Astrophys. 334, 558-570 (1998)
On the nature of the Be phenomenon
I. The case of Canis Majoris
P. Harmanec
Astronomical Institute, Academy of Sciences, CZ-251 65
Ond ejov, Czech Republic
(hec@sunstel.asu.cas.cz, hec@mbox.cesnet.cz)
Received 6 August 1997 / Accepted 30 January 1998
Abstract
The main purpose of this paper is to demonstrate the extreme
complexity of the observed variations of Be stars on the example of a
well-observed bright Be star CMa. A
detailed analysis of all published radial velocities and a
representative set of photometric and spectral observations of this
star led to the following firm conclusions:
- At least three and possibly four different time scales of
variability of
CMa, ranging from 1
37 to more than 40 years, could be
identified.
- The correct mean period of the RV and line-profile changes
is 1
371906, not 1 3667 as
derived earlier.
- The brightness of the object and the strength of the Balmer
emission vary in an apparent cycle of several thousands of days. The
long-term brightness and emission-line changes can be understood as
consequences of the formation and gradual dispersal of a gaseous
envelope which is flattened and seen more face-on than equator-on.
During each episode, the envelope grows from an optically thick
pseudophotosphere to a more extended and optically thin envelope.
- Existence of much smaller episodes of light brightening which can
have the same cause (though on a more limited scale) has clearly been
demonstrated.
- The amplitude of the 1
37 RV curve varies on
a time scale somewhere between 10 and 300 d.
The following conclusions are less certain and represent possible
alternatives to be tested by future, systematic and homogeneous
observations:
- Some evidence is presented that the amplitude of the 1
372 RV variations, local mean RV and brightness
of the object, prewhitened for the long-term changes, all vary on a
time scale of about 35 d, possibly with a period of 34
675.
- The O-C deviations of the local epochs of RV maxima from a linear
ephemeris for the 1
372 period seem to be
undergoing a slow and probably cyclic variation in time, being
shortest at times when the star is brightest and when a new Be
envelope begins to grow. However, the same O-C deviations can also be
reconciled with the 34 675 period. Whatever the
true timescale of the O-C deviations is, their behaviour can also be
simulated as an interference of several periods, the second most
significant period being close to 1 35. Several
reasons are given why the explanation in terms of one variable period
appears more probable.
- With the help of both, real and artificial data it is demonstrated
that the slow variation of the 1
3719 period -
if unrecognized - may be misinterpreted for a multiperiodic variation
with several close periods between 1 3 and 1
45. This constitutes a methodological warning
for the period analyses of data on some
Cep, Be and "slowly pulsating" B stars.
- The cause(s) of the variations with the 1
37
(and 1 345) period(s) and/or the 35 d cycle
remain unexplained. It is obvious, however, that these three periods
are not mutually independent. The 34 675 period
may be either a real physical period or a beat period between the 1
372 and 1 345 periods. In
the former case, CMa could be a 34
7 binary in an eccentric orbit and the periods
twice longer than the two periods near 1 4 would
represent the sidereal and synodic rotational periods of the Be
primary.
- Finally, some speculations are offered in terms of a hierarchical
multiple system of three or even four stars.
Key words: stars: emission-line,
Be
binaries:
eclipsing
stars: individual: ! CMa, HR 2733
Send offprint requests to: P. Harmanec
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© European Southern Observatory (ESO) 1998
Online publication: May 15, 1998
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