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Rotational Raman scattering in the Earth's atmosphere ... - SRON

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4<br />

Accurate model<strong>in</strong>g of spectral f<strong>in</strong>e-structure <strong>in</strong><br />

Earth radiance spectra measured with <strong>the</strong><br />

Global Ozone Monitor<strong>in</strong>g Experiment<br />

This chapter has been published as “Accurate model<strong>in</strong>g of spectral f<strong>in</strong>e-structure <strong>in</strong> Earth radiance spectra<br />

measured with <strong>the</strong> Global Ozone Monitor<strong>in</strong>g Experiment” <strong>in</strong> Appl. Opt. 46, 243–252 (2007) and was<br />

co-authored by O. P. Hasekamp and J. Landgraf.<br />

Abstract<br />

We present what we believe to be a novel approach to simulat<strong>in</strong>g <strong>the</strong> spectral f<strong>in</strong>e-structure<br />

(< 1 nm) <strong>in</strong> measurements of spectrometers such as <strong>the</strong> Global Ozone Monitor<strong>in</strong>g Experiment<br />

(GOME). GOME measures <strong>the</strong> Earth’s radiance spectra and daily solar irradiance spectra from<br />

which a reflectivity spectrum is commonly extracted. The high-frequency structures conta<strong>in</strong>ed<br />

<strong>in</strong> such a spectrum are, apart from atmospheric absorption, caused by <strong>Raman</strong> <strong>scatter<strong>in</strong>g</strong> and by<br />

a shift between <strong>the</strong> solar irradiance and <strong>the</strong> Earth’s radiance spectrum. Normally, an a priori<br />

high-resolution solar spectrum is used to simulate <strong>the</strong>se structures. We present an alternative<br />

method <strong>in</strong> which all <strong>the</strong> required <strong>in</strong>formation on <strong>the</strong> solar spectrum is retrieved from <strong>the</strong> GOME<br />

measurements. We <strong>in</strong>vestigate two approaches for <strong>the</strong> spectral range of 390–400 nm. First, a<br />

solar spectrum is reconstructed on a f<strong>in</strong>e spectral grid from <strong>the</strong> GOME solar measurement. This<br />

approach leads to undersampl<strong>in</strong>g errors of up to 0.5% <strong>in</strong> <strong>the</strong> model<strong>in</strong>g of <strong>the</strong> Earth’s radiance<br />

spectra. Second, a comb<strong>in</strong>ation of <strong>the</strong> solar spectrum and one of <strong>the</strong> Earth’s radiance measurements<br />

is used to retrieve <strong>the</strong> solar spectra. This approach effectively removes <strong>the</strong> undersampl<strong>in</strong>g<br />

error and results <strong>in</strong> residuals close to <strong>the</strong> GOME measurement noise of 0.1%.<br />

4.1 Introduction<br />

In 1995, <strong>the</strong> European Space Agency launched <strong>the</strong> Global Ozone Monitor<strong>in</strong>g Experiment (GOME)<br />

[Bednarz, 1995, Fletcher and Lodge, 1996, Burrows et al., 1999b] on <strong>the</strong> second European Remote<br />

Sens<strong>in</strong>g satellite (ERS-2) <strong>in</strong> a sun-synchronized near-polar orbit. Its goal was to determ<strong>in</strong>e <strong>the</strong> concentration<br />

of several trace gases <strong>in</strong> <strong>the</strong> Earth’s <strong>atmosphere</strong> with a global coverage over a three-day

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