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Chapter IX General Conclusion<br />

Chapter IX<br />

General Conclusion<br />

As it has been already discussed in the present thesis, KDP crystals<br />

play very prominent role in NLO applications. In India, majority of research<br />

is carried out on characterization of NLO materials crystals, nevertheless,<br />

only few research work is reported on the device applications. It is<br />

interesting to note that in Raja Ramanna Centre for Advanced Technology<br />

(RRCAT), Indore, the growth of 75 x 75 x 125 mm 3 KDP crystals is<br />

reported. The optical homogeneity of KDP crystals was assessed by<br />

Mach-Zahnder interferometer [1, 2]. The elctro-optic modulator using<br />

DKDP crystal has been fabricated at RRCAT. Moreover, Type-II SHG cell<br />

using KDP, with clear aperture of 50 mm and length of 25 mm have been<br />

devised at the same institute for doubling Nd:YAG laser.<br />

There are certain characterizations based on very simple techniques<br />

but provide very interesting information. Michelson interferometer has<br />

been used for imaging the surface micro-morphology of prismatic and<br />

pyramidal faces of KDP. The spiral growth mechanism, which has been<br />

discussed in chapter – II, has been imagined in form of concentric fringes<br />

of equal thickness. These fringes originated from the screw dislocation -<br />

generated hillocks on the crystal face were discussed [3].<br />

Another technique employed to study the convection during the growth<br />

of KDP crystals is the Shadow-graphy. This technique was employed to<br />

map convection around growing crystal. The shadow-graph images are<br />

helpful to quantify the free convection in terms of Grashof number and<br />

332

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