1989
DOI: 10.1029/jd094id06p08339
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SAGE II inversion algorithm

Abstract: This paper provides a detailed description of the current operational SAGE II multichannel data inversion algorithm implemented at NASA Langley Research Center, Hampton, Virginia. This algorithm is compared to an independently developed inversion algorithm from the Laboratory of Atmospheric Optics, University of Lille, Lille, France. Inverted aerosol and ozone profiles from these two algorithms are shown to be similar within their respective uncertainties.

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Cited by 284 publications
(208 citation statements)
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“…[28] Slant columns of NO 2 are calculated from the 448 nm and 453 nm channels using a differential technique [Chu and McCormick, 1989]. Vertical profiles are then retrieved between 15 km and 60 km using an onion peeling procedure, where the NO 2 slant columns are smoothed prior to peeling.…”
Section: Sage II Instrumentmentioning
confidence: 99%
“…[28] Slant columns of NO 2 are calculated from the 448 nm and 453 nm channels using a differential technique [Chu and McCormick, 1989]. Vertical profiles are then retrieved between 15 km and 60 km using an onion peeling procedure, where the NO 2 slant columns are smoothed prior to peeling.…”
Section: Sage II Instrumentmentioning
confidence: 99%
“…Furthermore, different quantities may be implied as, for instance, the mean radius ro, the standard deviation ln(s), or the refractive index rt r. This could require the selection of a different order for the inversions, i.e., vertical first, spectral second [see Chu et al, 1989], for which the amount of work has to be compared with respect to the gained accuracy. Indeed, in this approach, which has been implemented by the LOA group in order to validate the SAGE II generic algorithm, the total extinction coefficient is computed first for each stratospheric layer before the species separation.…”
Section: Discussionmentioning
confidence: 99%
“…Therefore the difficult problem of determining the optimal regularization for an underlying unknown distribution is replaced by a simple smoothness constraint on its integral which is easily verified by a polynomial. Once again, we underline that the choice of a polynomial in X is arbitrary and that many other forms could be used, for instance, the one depending on ln(X) in the Laboratoire d'Optique Atmosph6rique (LOA) algorithm [see Chu et al, 1989]. The main point is that the determination of the optimal R value is now irrelevant.…”
Section: The Interpolation Problemmentioning
confidence: 99%
“…A radiative transfer model [7] is used to calculate simulated limb radiances, with inputs from nearby SAGE II [8] ozone, aerosol, and NO 2 profiles, as well as NCEP temperature and pressure that accompany the SAGE files, so as to accurately model limb scattering radiances at the GOMOS measurement location, and characterize stray light signals. Radiance profiles were constructed at selected pixels relevant to the retrieval algorithm and compared to GOMOS measurements.…”
Section: Figure 2: Example Of Radiance Level Of Contamination By Stramentioning
confidence: 99%