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The absolute magnitudes are computed from the absolute
luminosity given in the tracks and the bolometric corrections computed
from stellar atmosphere models. For all the photometric systems
described in the following sections, we give the absolute magnitude,
, expressed in the Johnson band. Absolute magnitudes in the
other passbands can then be derived from the colour indices provided
in the files. Our adopted bolometric correction scale is that
described in Lejeune et al. (1998), defined in such a way to fit the
empirical scale of Flower (1996) instead of using the unique
calibration point of the Sun. Note that with this definition, we find
for the solar model of Kurucz (1992), a value
slightly different of that usually quoted for the Sun.
The zero-points of the colours are defined from the Vega model
spectrum of Kurucz (1992); for the (UBV)
(RI)
JHKLL
M, the CMTT, and the
HST-WFPC2 photometric systems, the computed colours for this model are
set to zero, while for the Geneva system these values are adjusted on
the observed photometry of Vega, , ,
, , , and (Rufener
1976), and
Next: (UBV)(RI) JHKLLM
Up: Synthetic photometry
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Thibault Lejeune
2000-11-23