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

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1<br />

Introduction<br />

1.1 Observ<strong>in</strong>g skylight<br />

Look<strong>in</strong>g through an airplane w<strong>in</strong>dow one can admire <strong>the</strong> deep blue color of <strong>the</strong> sky. This blue color<br />

arises from molecules <strong>in</strong> <strong>the</strong> Earth’s <strong>atmosphere</strong>, of which <strong>the</strong> most abundant species <strong>in</strong> <strong>the</strong> dry <strong>atmosphere</strong><br />

are: nitrogen (N 2 ; volume mix<strong>in</strong>g ratio of 78.09%), oxygen (O 2 ; 20.95%), and argon (Ar;<br />

0.93%). These molecules, which have diameters that are more than a thousand times smaller than<br />

<strong>the</strong> wavelength of <strong>the</strong> <strong>in</strong>cident sunlight, scatter sunlight <strong>in</strong> all directions [M<strong>in</strong>naert, 2004]. Light with<br />

short wavelengths (i.e blueish light) is more strongly scattered than light with longer wavelengths.<br />

The human eye conta<strong>in</strong>s two groups of light receptor cells, <strong>the</strong> rods and cones. The rods are sensitive<br />

to dim light and mediate coarse black and white vision. The cones are specialized for daylight and<br />

come <strong>in</strong> three types 1 that mediate detailed color vision [Stockman and Sharpe, 2000]. When look<strong>in</strong>g<br />

at <strong>the</strong> sky <strong>the</strong> cones that are most sensitive to blue light are triggered more than <strong>the</strong> ones that predom<strong>in</strong>antly<br />

sense blueish-green and yellowish-green light. This <strong>in</strong>formation is sent to <strong>the</strong> bra<strong>in</strong> where <strong>the</strong><br />

image of a blue sky is formed [Kandel et al., 1991].<br />

Over <strong>the</strong> past centuries a plethora of <strong>in</strong>struments has been developed that complement our eyes and<br />

bra<strong>in</strong>s. Sir Isaac Newton (1643–1727) demonstrated with a simple glass prism that light is composed<br />

of different colors. Spectrometers can be built that accurately measure this, i.e. <strong>the</strong> <strong>in</strong>tensity of light<br />

as a function of wavelength. It was found that visible light covers only a small part (400–700 nm) of<br />

<strong>the</strong> whole spectrum of electromagnetic radiation. Development of new detector technology enabled<br />

humans to study spectra of <strong>in</strong>visible radiation as well. Dur<strong>in</strong>g <strong>the</strong> last decades of <strong>the</strong> twentieth century<br />

satellites have been launched with spectrometers on board. These space-borne spectrometers act as<br />

artificial ‘eyes <strong>in</strong> <strong>the</strong> sky’ that monitor <strong>the</strong> Earth from above. Unlike our eyes that conta<strong>in</strong> three types<br />

of spectral detectors 2 , many of <strong>the</strong>se spectrometers conta<strong>in</strong> several thousand different spectral detectors<br />

that toge<strong>the</strong>r cover a similar wavelength range as <strong>the</strong> human eye. Examples of such space-borne<br />

spectrometers are <strong>the</strong> Global Ozone Monitor<strong>in</strong>g Experiment and its successor (GOME and GOME-2),<br />

<strong>the</strong> Scann<strong>in</strong>g Imag<strong>in</strong>g Absorption Spectrometer for Atmospheric Chartography (SCIAMACHY), and<br />

<strong>the</strong> Ozone Monitor<strong>in</strong>g Experiment (OMI). Table 1.1 lists several properties of <strong>the</strong>se spectrometers.<br />

1 Approximately 8% of <strong>the</strong> male readers of this <strong>the</strong>sis has effectively two types of cones and is thus color bl<strong>in</strong>d.<br />

2 The spectral responses of <strong>the</strong> three types of detectors <strong>in</strong> <strong>the</strong> human eye (<strong>the</strong> S, M and L cone) show a maximum near<br />

442 nm, 543 nm and 570 nm, and have a full width at half maximum of 57 nm, 85 nm, and 111 nm, respectively [Stockman<br />

and Sharpe, 2000].

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