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Astron. Astrophys. 354, L13-L16 (2000)
1. Introduction
The hot subdwarf B (sdB) stars are low-mass stars
( ) located near the extreme horizontal
branch (Heber et al., 1984; Heber, 1986). Their helium (He) core,
feeding the 3 -cycle nuclear fusion, is
surrounded by a thin hydrogen (H) envelope
( ).
Following spectroscopic and photometric studies several classification
schemes can be found for the hot sds in general. According to Moehler
et al. (1990b), the sdBs are He-poor stars which display optical
spectra dominated by strong broad Balmer lines and weak, or absent,
HeI absorption. A compilation of about 1200 hot sds can be found in
Kilkenny et al. (1988). The hot subdwarfs represent in an emphasized
way the classical horizontal branch problem, namely: how can a red
giant of a given mass lose a substantial fraction of its H-rich
envelope at or soon after the He ignition in its core? (Jeffery and
Pollacco 1998). In the course of their evolution, a fraction of the
hot sds is expected to form white dwarf (WD) stars with lower than
average masses (Heber, 1986). Hence, a study of such stars is
extremely important from an evolutionary point of view. The discovery
that 13 sdB stars pulsate (O'Donoghue et al. 1999) has rapidly
increased the interest of the astronomical community for these
objects, since their interior can now be probed by seismological
investigation. At about the same time of their discovery,
investigations of the pulsational instability of the sdB stars were
reported by Charpinet et al. (1996), the pulsation driving mechanism
being due to an opacity bump associated with iron ionization. The
observational properties of the sdB pulsating stars (called EC 14026
stars from the prototype EC 14026-2647, Kilkenny et al. 1997) are the
following: periods between about 1 and 10 min, amplitudes between a
few millimag to a few hundredths of mag. In addition at least 5 of
them out of 13 are in binary systems (O'Donoghue et al. 1999). This
percentage is not far from the 40-50
binarity rate for the hot subdwarf population (Ulla and Thejll 1998
and references therein); therefore it is unlikely, but not impossible,
that binary companions play a direct role in the sdB pulsations. The
oscillation properties of sdB models, now rapidly growing (Charpinet
et al. 1997; Fontaine et al. 1998; O'Donoghue et al. 1998) predict
that both radial and nonradial modes should have about same
frequencies. It is possible, in principle, to distinguish between
radial and nonradial modes: nonradial modes are affected by stellar
rotation (they produce multiplets of almost equally spaced
frequencies), whereas radial modes are not. The seismological
investigation of the sdB stars could permit us to learn important
details about their inner structure and chemical composition, as has
been successfully done for several WD and pre-WD stars (Bradley 1998).
Moreover, with long term measurements (months-years), we can hope to
detect the variation of the pulsation period with time, which is
directly related to the evolutionary changes of stellar structure.
Within the framework of our monitoring program of a hundred hot
subdwarfs, in order to find eventual periodicities, in this letter we
will present the results obtained for the sdB star PG 0856+121
( =
;
=
by
Colin et al. 1994). PG 0856+121 was classified as a typical sdB star
by Moehler et al. (1990a) on the basis of its spectrum. The star does
not show evidence of binarity, such as the IR CaII triplet and
photometric red excess (Jeffery and Pollacco 1998). Moreover the
radial velocity is constant (Saffer
et al. 1998) and the significance of the IR excess found for this
object in the JHK bands by Ulla and Thejll (1998) does not
reach a 2 level for all the three
bands. The Strömgren photometry performed by Moehler et al.
(1990a) gave ,
, ,
. Wesemael et al. (1992) found
photometric values in fairly good accordance with those obtained by
Moehler et al. (1990a). Moehler et al. (1990b), from spectroscopy and
photometry, derived ,
,
pc and pc (distance from the
galactic plane). Saffer et al. (1994) from optical spectrophotometry
found fairly different values for temperature
( ) and surface gravity
( ). This fact renders evident the
difficulty in determining the temperature of such stars using colour
indices, independently of the photometric system used, since the
central wavelength of the filters employed lies in the red-wing of the
Planckian distribution, as also pointed out by Wesemael et al.
(1992).
© European Southern Observatory (ESO) 2000
Online publication: January 31, 2000
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