Films minces à base de Si nanostructuré pour des cellules ...
Films minces à base de Si nanostructuré pour des cellules ...
Films minces à base de Si nanostructuré pour des cellules ...
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Inelastic (Raman and Brillouin) scattering. A part of the photons is re-radiated<br />
at the inci<strong>de</strong>nt energy and this is known as Rayleigh scattering. Few photons are<br />
scattered due to interaction with optical and acoustical phonons in the material<br />
and are termed as Raman and Brillouin scattering respectively. The energy shift of<br />
the Raman scattered light towards high (Anti-stokes) and low (Stokes) frequencies<br />
yield information on the vibrational mo<strong>de</strong>s in the measured sample. Figure 2.11<br />
illustrates the Raman shift of the scattered light.<br />
tel-00916300, version 1 - 10 Dec 2013<br />
Figure 2.11: Illustration of scattering of light and Raman shift.<br />
Experimental set-up and working<br />
A Raman system typically consists of four major components:<br />
ˆ Excitation source (Laser),<br />
ˆ Sample illumination system and light collection optics,<br />
ˆ Wavelength selector (Filter or Spectrophotometer),<br />
ˆ Detector (Photodio<strong>de</strong> array, CCD or PMT).<br />
The schematic diagram of a Raman spectrometer is as shown in gure 2.12.<br />
The sample un<strong>de</strong>r investigation is illuminated with a laser beam. The scattered<br />
light is collected with a lens and is sent through a notch lter which removes the<br />
scattered light that is of the frequency of the laser beam. Only the light that has an<br />
energy shift (Raman shifted light) passes through the lter. The movable grating<br />
disperses the light and the dierent wavelengths are collected by a charged couple<br />
<strong>de</strong>vice (CCD) camera. Raman spectrometer from Jobin Yvon equipped with Ar<br />
44