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Updates to STIS Spectroscopic Throughputs
On 2005-Apr-04, a number of new photometric throughput (pht) and
time-dependent sensitivity (tds) reference files were delivered
that provide significant improvements to the absolute flux
calibration for 1D extractions of STIS low-dispersion, PRISM, and
echelle modes.
Throughputs for G140L and G230L have increased by about 2% at most
wavelengths (thereby giving extracted fluxes that are lower by about
2%), with somewhat larger changes at the shortest wavelengths of each
grating and in the vicinity of the Lyman-alpha line.
Throughputs for CCD gratings have not changed with this
release. Once corrections for time-dependent-sensitivity (TDS)
changes and charge transfer inefficiencies (CTI) are made, the
absolute flux accuracy for all STIS low-dispersion observations done
using the 52X2 aperture should have relative accuracies of 3% or
better and an absolute accuracy of better than 5% (see discussion in
Bohlin et al. 2000, AJ 120,437).
For E140H and E140M the new sensitivities are typically 3 to 20%
higher, with substantially larger changes at the very shortest
wavelengths near 1140 Angstroms. E230H and E230M sensitivities are
changed by less than 10% at most wavelengths. TDS corrections are
now included for all echelle observations, and for echelle
observations using primary wavelength settings and the 0.2X0.2
aperture, typical flux accuracy should be ~5%, although isolated
individual observations may occasionally be sufficiently miscentered
in the 0.2X0.2 aperture to have a more noticeable flux loss.
The new NUV MAMA PRISM throughput curves differ from the previous
ones by up to 15%, and extracted x1d PRISM fluxes now also include
TDS corrections. The absolute accuracy of these observations should
now be about 5%. A new and more accurate photometric correction
table (pct file) which corrects the flux for the vertical extent of
the chosen extraction region has also been delivered. An error in
the previous prism pct file, which could cause errors in 1D-extracted
fluxes of up to 25% for slitless PRISM data, has been corrected.
Note that there are a number of issues for the calibration of
extracted fluxes for point source spectra that have yet to be fully
addressed.
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For the CCD gratings there is some vignetting as a function of
position along the slit that is not yet taken into account.
This can cause wavelength dependent flux errors of up to 5% for
spectra not placed near the central rows of the detector.
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The current calibration software assumes that the grating and
aperture throughputs can be determined separately and then
multiplied in any combination. This is apparently not true for
the G430L and G750L gratings, which contain extra Lyot stops
that appear to make the grating throughputs aperture
dependent. For the 52X0.2 and 52x0.2E1 apertures, this can
lead to flux errors of as much as 10%, and can create
discontinuities of 2 to 6% in the overlap regions between
different gratings.
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At the shortest wavelengths of each first-order grating, the
sensitivity function varies rapidly near the blocking filter
cutoff, and small wavelength misalignments can cause flux
errors of order 10%.
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The secondary wavelength settings for the echelles still use
pre-launch estimates for the blaze function and do not yet
include corrections for shifts of the blaze function with
respect to the wavelength scale between different observations.
These effects can result in significant distortion of the
relative fluxes within each spectral order. However, this new
pht and tds file delivery will yield improved mean fluxes even
for these secondary settings.
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The implemented sensitivity curves for the first-order medium
resolution settings are of varying quality and have not yet
been fully updated using all available standard star
observations. While most first order medium resolution central
wavelength settings are accurate to 3% or better, a few show
anomalies at the 5 to 10% level, including a few that may mimic
spectral features (e.g., the G230MB 2135 setting has a spurious
20 Angstrom wide 5% deep dip in the calibrated fluxes). Those
wavelengths defined as secondary settings and E140M
observations taken after the 1999-Mar shift of FUV-MAMA
spectra to a position with lower dark current are especially in
need of improvement.
We hope to address most of the above issues in the next few months
and deliver a final flux calibration for 1D spectral extractions
by the end of the year.
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