Rotational Raman scattering in the Earth's atmosphere ... - SRON
Rotational Raman scattering in the Earth's atmosphere ... - SRON
Rotational Raman scattering in the Earth's atmosphere ... - SRON
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16 Chapter 1<br />
The answers to <strong>the</strong>se questions are given <strong>in</strong> Chapters 2 and 3, respectively. In Chapter 2 we present<br />
a model approach that is based on <strong>the</strong> doubl<strong>in</strong>g-add<strong>in</strong>g method. The power of this approach is that<br />
<strong>the</strong> multiple scattered radiation, both elastically and <strong>in</strong>elastically scattered, is obta<strong>in</strong>ed <strong>in</strong> a straightforward<br />
way. One starts with <strong>the</strong> analytical s<strong>in</strong>gle <strong>scatter<strong>in</strong>g</strong> solution and uses <strong>the</strong> extended doubl<strong>in</strong>gadd<strong>in</strong>g<br />
equations to obta<strong>in</strong> <strong>the</strong> multiple scattered radiation. With this scalar model <strong>the</strong> approximation<br />
of <strong>in</strong>clud<strong>in</strong>g only one order of <strong>Raman</strong> <strong>scatter<strong>in</strong>g</strong> is <strong>in</strong>vestigated.<br />
Chapter 3 describes a different approach where <strong>the</strong> effect of <strong>in</strong>elastic <strong>Raman</strong> <strong>scatter<strong>in</strong>g</strong> is described<br />
by a perturbation to <strong>the</strong> radiative transfer problem which <strong>in</strong>cludes multiple Rayleigh <strong>scatter<strong>in</strong>g</strong>.<br />
Here, <strong>the</strong> perturbation series describes <strong>in</strong>creas<strong>in</strong>g orders of <strong>Raman</strong> <strong>scatter<strong>in</strong>g</strong>. For numerical<br />
implementation <strong>the</strong> perturbation series is truncated at first order, which means that one order of <strong>Raman</strong><br />
<strong>scatter<strong>in</strong>g</strong> is <strong>in</strong>cluded <strong>in</strong> addition to multiple elastic <strong>scatter<strong>in</strong>g</strong>. This eases <strong>the</strong> implementation<br />
and results <strong>in</strong> a very efficient vector radiative transfer model <strong>in</strong>clud<strong>in</strong>g <strong>in</strong>elastic <strong>Raman</strong> <strong>scatter<strong>in</strong>g</strong>.<br />
With this model <strong>the</strong> impact of <strong>the</strong> scalar approximation on <strong>the</strong> reflectivity spectrum <strong>in</strong>clud<strong>in</strong>g <strong>the</strong><br />
R<strong>in</strong>g effect can be <strong>in</strong>vestigated.<br />
Accurate simulation of <strong>the</strong> R<strong>in</strong>g effect relies heavily on <strong>the</strong> use of an accurate <strong>in</strong>put solar spectrum.<br />
The R<strong>in</strong>g effect that is <strong>in</strong>duced by <strong>the</strong> solar Fraunhofer l<strong>in</strong>es is directly l<strong>in</strong>ked to <strong>the</strong> exact<br />
amplitude and spectral shape of <strong>the</strong> Fraunhofer l<strong>in</strong>es <strong>in</strong> <strong>the</strong> solar spectrum. In <strong>the</strong> literature it is common<br />
to rely on a reference solar spectrum. However, large deviations exist between <strong>the</strong>se reference<br />
solar spectra [Gueymard, 2004]. In addition, <strong>the</strong>se spectra show significant differences with <strong>the</strong> solar<br />
spectra measured by <strong>in</strong>struments such as GOME, SCIAMACHY, OMI and GOME-2 (e.g. Fletcher<br />
and Lodge [1996]). This raises <strong>the</strong> question:<br />
3. S<strong>in</strong>ce <strong>the</strong> <strong>in</strong>put solar spectrum is so crucial for <strong>the</strong> simulation of <strong>the</strong> R<strong>in</strong>g effect, what is <strong>the</strong> best<br />
model<strong>in</strong>g approach?<br />
In Chapter 4 we describe a newly developed approach <strong>in</strong> which <strong>the</strong> maximum amount of <strong>in</strong>formation<br />
that is conta<strong>in</strong>ed <strong>in</strong> <strong>the</strong> daily measured solar spectrum is employed to simulate <strong>the</strong> spectral f<strong>in</strong>estructure<br />
<strong>in</strong> <strong>the</strong> reflectivity measurements <strong>in</strong>stead of rely<strong>in</strong>g on a reference <strong>in</strong>put solar spectrum.<br />
The R<strong>in</strong>g effect <strong>in</strong> <strong>the</strong> measurement is sensitive to presence of clouds (e.g Jo<strong>in</strong>er and Bhartia<br />
[1995], de Beek et al. [2001]) and aerosols (e.g Stam et al. [2002], Langford et al. [2007]) <strong>in</strong> <strong>the</strong><br />
observed scene. The cloud <strong>in</strong>formation that can be retrieved from <strong>the</strong> R<strong>in</strong>g effect, such as cloud top<br />
height, can be used to improve trace gas retrievals for cloudy scenes. This is important s<strong>in</strong>ce most of<br />
<strong>the</strong> GOME, SCIAMACHY, OMI and GOME-2 observations are <strong>in</strong>fluenced by clouds due to <strong>the</strong> large<br />
field-of-view of <strong>the</strong> considered spectrometers (see footpr<strong>in</strong>t size <strong>in</strong> Table 1.1). Two o<strong>the</strong>r approaches<br />
are commonly used <strong>in</strong> <strong>the</strong> literature for <strong>the</strong> same purpose, but <strong>the</strong>se are based on us<strong>in</strong>g absorption<br />
features of oxygen and <strong>the</strong> oxygen dimer <strong>in</strong> <strong>the</strong> reflectivity spectrum, i.e. <strong>the</strong> O 2 A band near 760 nm<br />
and absorption by O 2 -O 2 at 477 nm. In <strong>the</strong> last chapter, Chapter 5, we consider <strong>the</strong> question:<br />
4. How does <strong>the</strong> capability to retrieve cloud parameters from <strong>the</strong> R<strong>in</strong>g structures compare with<br />
o<strong>the</strong>r commonly used approaches that use absorption bands of oxygen and <strong>the</strong> collisional complex<br />
of oxygen?<br />
The different approaches for <strong>the</strong> retrieval of cloud parameters are evaluated, and <strong>the</strong> most appropriate<br />
method is proposed for present and future GOME-type <strong>in</strong>struments.