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1. Introduction

The prototype of tex2html_wrap_inline1045Bootis stars was found by Morgan et al. (1943) and the group can be described as metal-poor PopulationI, A-type stars with no magnetic field larger than tex2html_wrap_inline1047. In a recent paper (Paunzen et al. 1997) we have reviewed the various classification criteria and have established a homogeneous group of tex2html_wrap_inline1049Bootis stars. Although tex2html_wrap_inline1051Bootis stars occupy the same parameter space in a Hertzsprung-Russell-diagramme as do "normal" A-type and some peculiar (CP1, cool CP2) stars, they are distinguished e.g. by results of high resolution spectroscopy and UV observations.
The evolutionary status of tex2html_wrap_inline1053Bootis stars is still controversial. The two theories discussed in the literature involve diffusion, either in combination with accretion of interstellar matter as in post-AGB stars (Turcotte & Charbonneau 1993), or with mass loss (Michaud & Charland 1986).
With the tools of asteroseismology it is in principle possible to investigate the evolutionary status and internal structure of a star from its pulsation frequency spectrum. We therefore have started a photometric survey for pulsation among tex2html_wrap_inline1055Bootis stars in 1993. Eight observing runs were at least partly dedicated to this survey so far (Table2 (click here)). Up to now we have found 13 new pulsating members of this group (Weiss et al. 1994; Paunzen & Handler 1996 and references therein). Frequencies (6 to 45dtex2html_wrap_inline1057) and amplitudes suggest a close connection to tex2html_wrap_inline1059Scuti stars.
The main theoretical framework to describe tex2html_wrap_inline1061Scuti pulsation is well developed, although the effects of diffusion and low metallicity on pulsation are not conclusively investigated yet. A comparison of the CP1 and tex2html_wrap_inline1063Bootis stars is especially interesting. For both groups, diffusion seems to be the main mechanism responsible for the overabundance (CP1) as well as for the underabundance of metals (tex2html_wrap_inline1065Bootis stars). However, the first group consists of typically nonvariable stars (Alecian 1996), which is not the case for the second group.
Some preliminary null results of our survey have been published in a series of IBVS-notes (Kuschnig et al. 1996; Paunzen et al. 1996a,b). In this paper we present all data on "constant" stars, in the sense that we are able to give an upper limit for a possible variability. For each set of differential data we have computed a Fourier spectrum (Figs. 4 (click here)a to 4 (click here)c).

   Table 1: Observation log and results for the observed stars

  Table 1: continued


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