Two light intensity modulators have been constructed using LiTaO3 and LiNbO3, respectively, in a reentrant microwave cav ity tuned to 4.2 GHz. The loop-coupled cavity is shown sche matically in Fig. 1. The crystal is attached to the chisel-shaped center post with silver paste and is oriented so that the (peak) voltage V is along the c axis. The cavity diameter D is 1.91 cm, the post diameter d is 0.38 cm and the resonant frequency is deter mined by the cavity height h. Not all the electric field is concentrated in the gap containing the crystal. A rough estimate of the added capacity Ca in paral lel with the crystal is ε0πD/4h. The ratio of total capacity CT to crystal capacity C is then
[1]
G. D. Boyd,et al.
OPTICALLY‐INDUCED REFRACTIVE INDEX INHOMOGENEITIES IN LiNbO3 AND LiTaO3
,
1966
.
[2]
Lithium Tantalate Light Modulators
,
1967
.
[3]
I. Kaminow,et al.
Propagation characteristics of partially loaded two-conductor transmission line for broadband light modulators
,
1963
.
[4]
I P Kaminow,et al.
Electrooptic light modulators.
,
1966,
Applied optics.
[5]
E. Turner,et al.
HIGH‐FREQUENCY ELECTRO‐OPTIC COEFFICIENTS OF LITHIUM NIOBATE
,
1966
.
[6]
I. Kaminow.
Strain Effects in Electrooptic Light Modulators
,
1964
.