It is generally accepted that sdB stars can be identified with models of the extended Horizontal Branch (EHB) burning He in their core (Heber 1986; Saffer et al. 1994). The hydrogen envelope surrounding the core of about half a solar mass is very thin (<2 % by mass) and therefore inert. These EHB stars will continue their evolution directly towards the white dwarf graveyard avoiding the AGB and planetary nebula phases (Dorman et al. 1993).
How sdB stars evolve towards the EHB with effective temperatures of up to
40 000 K remains a puzzle. The star must have lost all but a tiny fraction of
the hydrogen envelope at the same time as the He core has attained the minimum
mass (0.5
)
required for the He flash. This challenges every
mass loss mechanism in aspects of timing and effectivity. Recent findings
(Maxted et al. 2001; Saffer et al. 2001; Heber et al.
2002a) emphasize the significance of close binary evolution.
Some of the sdB stars were recently found to exhibit rapid multi-periodic light
variations (
80-600 s) of low amplitudes (a few mmag). They form
a new class of pulsating stars named after the prototype EC 14026 stars
(Kilkenny et al. 1997). Since then a relatively large number of new sdB pulsators
has been discovered. 31 are known today (Charpinet 2001; Piccioni et al. 2000; Silvotti et al. 2000). The
observed brightness variations are caused by radial and non-radial, low degree
and low order acoustic pulsation modes. The pulsations in these stars are driven
by an opacity bump due to Fe and other metallic species (Charpinet et al.
1997) at a temperature of
2
105 K in the sdB
envelope.
Stellar pulsations allow a direct insight into the structure of such stars and therefore into the evolutionary history. The frequencies or periods of the pulsation modes probe the chemical stratification and the mass which otherwise are difficult or even impossible to determine. The power of asteroseismological tools has been demonstrated in the field of pulsating white dwarfs for which stellar parameters like mass, luminosity or thickness of the envelope were derived (e.g. Winget et al. 1991). In the case of variable sdB stars these parameters will constrain the evolutionary history and consequently shed more light on the origin of these stars.
Identification of pulsation modes (characterized by spherical harmonics with
the indices l and m) is a prerequisite for asteroseismology. Brassard et al.
(2001) have successfully carried out an asteroseismological analysis
for PG 0014+067. For the first time they were able to determine the stellar
mass (
)
as well as the envelope mass
(
)
and both are in
excellent agreement with predictions from evolutionary models (Dorman et al.
1993).
Pulsations produce not only photometric variations but also line profile
variations that offer an alternative approach towards mode identification.
PG 1605+072 is the ideal target for this application: it has the longest
pulsation periods (500 s) which enables spectra with reasonable S/N to be
obtained within each pulsation period. Moreover, this star has the largest
variations of all known sdBVs (0.2 mag in the optical) and by far the richest
frequency spectrum (>50 modes, Kilkenny et al. 1999). A recent
spectroscopic study revealed this star to be a rather rapid rotator
(
km s-1, Heber et al. 1999) which will complicate the
identification of modes due to non-linear effects on mode splitting.
This work presented here serves as a feasibility study in order to find out whether an asteroseismologic analysis of PG 1605+072 is possible. For this purpose we have done simultaneously time-series spectroscopy and multi-band photometry (observations and reductions in Sect. 2). The analysis of the results is presented in Sect. 3. Previously, other groups have done radial velocity studies (O'Toole et al. 2000, 2002; Woolf et al. 2002) or photometric campaigns (e.g. Kilkenny et al. 1999) on PG 1605+072. Simultaneous multi-band photometry has not been observed before. This enables us to study the temporal evolution of the frequencies and amplitudes of the pulsation modes (Sect. 4). Finally, we discuss our results and give a brief outlook to future work in Sect. 5.
Copyright ESO 2003