Astron. Astrophys. 354, 881-891 (2000)
6. The nature of the secondaries
6.1. Photometric evidence
The photometric analysis of the Am stars in the Hyades and Praesepe
shows several interesting facts. All the photometric data were taken
in the WEBDA (Mermilliod
1999 1)
compilation of literature. The Am stars are off the main relation for
normal stars by about 0.03 mag, in a
( , )
diagram (Fig. 16). The ( ) excess
results from the line-blanketing in the Am stars. In a coulour
magnitude diagram, part of the vertical distance to the ZAMS, usually
interpreted as a sign of duplicity, is due to the metallicity effect.
The parameter is preferred to
( ) because
is probably less sensitive to
metallicity.This effect offers an interesting possibility of
identifying Am stars in the main sequence of more distant clusters,
provided that the photometry has a precision of 0.01 mag and that the
clusters have no differential reddening.
![[FIGURE]](img111.gif) |
Fig. 16. The Am stars (open symbols) are clearly separated by about 0.03 mag from the sequence of normal stars.
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In a ( ,
) diagram (Fig. 17), where
is estimated from the apparent
magnitude and the distance of each open cluster (Mermilliod 1999), the
distribution of the Am stars is clearly bimodal. The double-lined
systems (open squares) are accordingly located on the binary ridge,
about 0.75 mag above the ZAMS, while most other systems are close to
or on the ZAMS. This implies that the secondaries are fainter than the
primaries by at least 3 to 4 magnitudes, which fixes an upper limit on
the secondary masses. The values for the masses derived from the
present data are given in Table 6.
![[FIGURE]](img113.gif) |
Fig. 17. The double-lined Am stars are nearly close to the binary ridge, as expected. Most single-lined binaries are close to or on the ZAMS. Small dots are Hyades non-Am stars.
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![[TABLE]](img115.gif)
Table 6. Minimum and maximum masses of the secondaries
6.2. Secondary masses
In Tables 3 and 4 the values of the mass function
are listed, and we have derived the
inclination for the synchronised binaries. We can therefore estimate
the masses of the secondaries (Table 6).
The three synchronised stars (KW 279, vB 38 and
vB 45) present quite similar masses of the secondary
( ) of about 0.5
. For KW 40 the difference
between , which is derived form the
photometry, and , calculated from
Vsync, results from the composition of two errors.
Firstly, the luminosity of KW 40 is not corrected from the third
component luminosity, and secondly, a small error on the
V value would result in a significant
change of the derived mass. A secondary mass of 1.81
would imply that the secondary is an
A-type star, which probably has a large rotational-velocity and might
not be detected by CORAVEL. For vB 169, the value of the
secondary mass can be affected by the presence of the third and fourth
components of the system.
The six systems not detected in X-rays have secondary masses
compatible with that of a white dwarf.
© European Southern Observatory (ESO) 2000
Online publication: February 25, 2000
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