Astron. Astrophys. 346, 243-259 (1999)
Appendix A: narrow band calibration
The narrow-band filters for IRAC2b are relatively broad
( µm), thus the line
and corresponding continuum filters share a large overlapping region.
For calibration, two strategies were used. The counts inside the
standard's PSF were determined by using an IDL adaption of the DAOPHOT
package by W. Landsman. Then the actual flux of HD169588 at the
desired wavelength was interpolated from the H and
fluxes given by Carter & Meadows
(1995). Each of the object frames was then multiplied by the ratio of
flux-to-counts at the corresponding wavelength. For flux measurements,
we also did a continuum subtraction. As the broadness of the filters
leads to a serious contamination of the continuum with line emission,
we had to take care of this. The flux per pixel in a line image is
given by:
![[EQUATION]](img141.gif)
is the measured
Br flux in the image. The symbol
" " means "at the point of". Thus
means the transmission of the line
filter at the wavelength of the line. As the images are already flux
calibrated, transmissions are measured relative to the transmission of
the line filter at the line's wavelength (i.e.
is 1 in this case).
is the flux of line photons
contributing to the total flux in the pixel, while
denotes the continuum flux. The
latter can of course also be present at different wavelengths while
the line is assumed to be so narrow that it virtually only exists at
. The flux in the continuum filter
should be given by:
![[EQUATION]](img148.gif)
When assuming and taking
, we can combine this to
![[EQUATION]](img151.gif)
These equations ignore the fact that only flux densities are
measured in finite filter widths, but since these widths are identical
for all the filters, the effect can be neglected. The factor
gives the ratio of the continuum
photon number at the two wavelengths considered. It was determined by
simultaneously minimising the fluxes of 5 selected field stars. To
determine the Br flux density, the
procedure was performed for two continuum filters (NB4 and NB7) with
variations in the resulting Br flux
below 4%. Together with another 4% uncertainty from background noise
in the resulting image and approximately 2% from the calibration using
the standard, we end up with a total flux uncertainty of 6%. For the
line, only NB4 was used for
calibration, because residual Br flux
in NB7 rendered the result useless.
© European Southern Observatory (ESO) 1999
Online publication: May 6, 1999
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