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Chapter V Dielectric Study of ……<br />

-<br />

at temperature from 70 to 79 o C, additional defects were created by breaking<br />

the stronger hydrogen bond in ammonium groups. At temperature above 97<br />

o C, ammonium ions in the crystal were proposed to have contributed for the<br />

electrical conduction.<br />

Recently, Ambujan [39] studied the effect of cation doping (Mg +2 , Cu +2 ,<br />

Ni +2 and Ca +2 ) in KDP crystals on their dielectric properties. The variation of<br />

dielectric constant with frequency suggested that as the frequency increased<br />

the dielectric constant decreased and at high frequency the leveling of the plot<br />

to the X-axis was observed. The pure KDP crystals exhibited the least values<br />

of dielectric constant. It was observed that due to change in the sizes of the<br />

metal dopant ions, there was change in the value of dielectric constant at any<br />

particular frequency. The polarizability was expected to increase as the ions<br />

were smaller and highly charged. Ambujan [39] could observe the increase in<br />

the value of dielectric constant of doped sample in accordance with the ionic<br />

radii of the metallic dopant.<br />

KDP crystallizes in tetragonal crystal system with space group 14 2d.<br />

The crystal structure consists of PO4 tetrahedral joined by four hydrogen<br />

bonds to neighboring PO4 tetrahedral in such a way that each PO4 tetrahedral<br />

has two hydrogen atoms associated with it giving (H2PO4) - ion. The PO4 group<br />

and K + ions are built up in such a way that K and P atoms alternate each<br />

other at a distance of c/2 along the c-axis. During the metal ion substitution<br />

the hydrogen bond in the structure break down giving rise to the loosening of<br />

the hydrogen and the creation of additional charged defects. These lattice<br />

defects cause the increased space charge contribution.<br />

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