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To obtain absolute accuracy better than a few parts in 106 from FT
spectra, it is necessary to determine a multiplicative correction to
the wavenumber scale from accurately known internal standard lines. This
correction is often specified by a factor, keff, such that
Here σc is the calibrated wavenumber and σu is
the uncalibrated wavenumber.
We have used seven Th I lines [DeGraffenreid & Sansonetti (2002)] measured by
optogalvanic laser spectroscopy in a low current Th-Ne hollow cathode
lamp. These lines, which lie between 13360 cm−1 and
14400 cm−1, have a reported uncertainty of 0.0002 cm−1 (1.4
parts in 108). The calibration derived from these lines
(Figure 1) gives a value of keff of
(7.20 ± 0.14)×10−7. The error bars are dominated by the
low signal-to-noise ratio in the FT spectrum at the extreme edge of
the bandpass. Because the calibration lines are limited to a narrow
region at the short wavelength end of our spectra, it is desirable to
have some check on the results in the long wavelength region to ensure
that the value of keff is actually constant across the region of
interest as expected from the theory of FT spectroscopy. Comparison
with results of [Engleman, Hinkle, & Wallace(2003)] provides such a check, and full details
are given in [Kerber et al.(2008)]. The spectrum optimized for
wavelengths above 2000 nm was calibrated from the spectrum optimized
for the region 800 nm to 2000 nm, with an total uncertainty in keff of
2x 10−8.
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