Astron. Astrophys. 351, 954-962 (1999)
2. Observations
2.1. The sample
We have chosen our sample from the list of Mathieu (1994). In
Paper I, Monin et al. already presented some spectroscopic
measurements on five objects in this list, with separations ranging
between and
. In this paper we present
complementary observations of closer binaries from the same list. This
new sample (see Table 1) now includes all the binaries new sample
(see Table 1) now includes all the binaries in this list with
separations ranging between and
, to the exception of HBC 411 (CoKu
Tau/3) and HBC 389 (Haro 6-10).
![[TABLE]](img16.gif)
Table 1. Complete list of spectroscopically observed binaries (Paper I and this paper). Listed are the Herbig & Bell (1988) catalogue numbers (hereafter: HBC) of the primary and secondary when available, the binary separation and the previous classification of the whole system as CTTS or WTTS (from HBC unless explicitly quoted).
Notes:
) resolved VRI imaging photometry was obtained for these objects
) Paper I
a) this work
b) Hartmann et al. (1991)
2.2. New spectroscopic observations
The observations were conducted on 1996 November 5 and 6, and
December 1, at the Canada-France-Hawaii Telescope on Mauna Kea. We
used the STIS2 detector with a
/pixel scale. Using SIS (Subarcsecond
Imaging Spectrograph) providing tip-tilt correction, we obtained an
angular resolution of about to
. Differential VRI imaging
photometry was also performed during the first two nights for some
targets. For each system, the primary has been defined as the
brightest star in the band.
Long-slit spectra were obtained using a 1" slit and a grism. The
usefull range of the spectra is 4000 to
Å, yielding a
Å/pixel scale. However, the
actual resulting spectral resolution is
Å, except for HBC 356-357 where
it is Å. Spectra of calibration
lamps and of a spectrophotometric standard (Feige 110) were obtained
every night. All spectra have been wavelength calibrated, cosmic-ray
cleaned, flat fielded, sky emission subtracted and flux calibrated.
All data reduction steps were performed with standard
IRAF 1 routines.
The two stellar spectra of each binary were deblended and extracted
using a task fitting two gaussians with the same FWHM profile. This
reduction procedure is accurate as long as the separation remains
larger than the seeing, which was the case for all our sources except
FX Tau and UY Aur, the closest systems of our sample (see Sect. 3.1
for details).
Our estimates of the spectral types are based on the strength of
TiO bands for M stars, and on relative strengths of CaI
6122,62, NaI
, CaH
6350,80 and CaH
6750-7050 for K stars. We used the
standard grids from Allen & Strom (1995) and Kirkpatrick et al.
(1991), and we also observed a series of spectral type standards
during the same nights as the binary targets. From these standard
stars measurements, we find that our estimates are accurate to within
one subclass for the whole sample. However, we are unable to determine
spectral types later than M5, because most of the spectral features we
use do not change anymore with effective temperature for such late
type stars. Spectra at longer wavelengths are needed for the
classification of the reddest objects.
Uncertainties on emission line equivalent widths (hereafter EWs)
were estimated by using the maximum and minimum acceptable continuum
values next to the lines. They are typically smaller than 5%, except
for the weakest lines, where they are of the order of 0.1-0.2 Å.
In the blue part of the spectrum, for the faintest stars,
uncertainties can reach 10-15%.
We evaluated differential photometry for 8 of our sources in the
VRI bands. Uncertainties are usually smaller than 0.02 mag and
never exceed 0.03 mag.
© European Southern Observatory (ESO) 1999
Online publication: November 16, 1999
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