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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

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