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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3<br />
A vector radiative transfer model us<strong>in</strong>g <strong>the</strong><br />
perturbation <strong>the</strong>ory approach<br />
This chapter has been published as “<strong>Rotational</strong> <strong>Raman</strong> <strong>scatter<strong>in</strong>g</strong> of polarized light <strong>in</strong> <strong>the</strong> Earth’s <strong>atmosphere</strong>:<br />
A vector radiative transfer model us<strong>in</strong>g <strong>the</strong> radiative transfer perturbation <strong>the</strong>ory approach” <strong>in</strong> J.<br />
Quant. Spectrosc. Radiat. Transfer 87, 399–433 (2004) and was authored by J. Landgraf and co-authored<br />
by O. P. Hasekamp, R. van Deelen and E. A. A. Aben.<br />
Abstract<br />
A plane-parallel vector radiative transfer model is presented to simulate <strong>the</strong> effect of rotational<br />
<strong>Raman</strong> <strong>scatter<strong>in</strong>g</strong> on radiance and polarization properties of sunlight reflected by <strong>the</strong> Earth <strong>atmosphere</strong><br />
<strong>in</strong> <strong>the</strong> ultraviolet and visible part of <strong>the</strong> solar spectrum. The model employs <strong>the</strong> radiative<br />
transfer perturbation <strong>the</strong>ory, which treats <strong>in</strong>elastic rotational <strong>Raman</strong> <strong>scatter<strong>in</strong>g</strong> as a perturbation<br />
to elastic Rayleigh <strong>scatter<strong>in</strong>g</strong>. The approach provides a perturbation series expansion for a simulated<br />
radiation quantity, where each term describes <strong>the</strong> effect of one additional order of <strong>Raman</strong><br />
<strong>scatter<strong>in</strong>g</strong>. The model is worked out <strong>in</strong> detail to first order. Here, <strong>the</strong> adjo<strong>in</strong>t formulation of radiative<br />
transfer reduces significantly <strong>the</strong> numerical effort of computational applications. Numerical<br />
simulations are presented for <strong>the</strong> ultraviolet part of <strong>the</strong> solar spectrum and <strong>the</strong> effect of <strong>Raman</strong><br />
<strong>scatter<strong>in</strong>g</strong> on <strong>the</strong> Stokes parameters I, Q and U of <strong>the</strong> reflected sunlight is studied. Fur<strong>the</strong>rmore,<br />
<strong>the</strong> accuracy of both <strong>the</strong> s<strong>in</strong>gle <strong>scatter<strong>in</strong>g</strong> approximation and <strong>the</strong> scalar radiative transfer<br />
approach is considered for <strong>the</strong> simulation of R<strong>in</strong>g structures. The use of <strong>the</strong>se approximation<br />
techniques is <strong>in</strong>vestigated for <strong>the</strong> simulation of R<strong>in</strong>g structures <strong>in</strong> polarization sensitive GOME<br />
measurements.<br />
3.1 Introduction<br />
Satellite measurements of backscattered sunlight <strong>in</strong> <strong>the</strong> ultraviolet and visible part of <strong>the</strong> solar spectrum<br />
conta<strong>in</strong> essential <strong>in</strong>formation about <strong>the</strong> composition of <strong>the</strong> <strong>atmosphere</strong>. In <strong>the</strong> years 1978-2002<br />
a series of Solar Backscattered Ultraviolet (SBUV) <strong>in</strong>struments were launched on NASA’s NOAA<br />
satellites, which measure <strong>the</strong> backscattered ultraviolet radiances at 12 wavelengths between 250–340