Electro−optic light modulation in a planar zinc−blende−type crystal waveguide

1975 ◽  
Vol 46 (1) ◽  
pp. 260-265 ◽  
Author(s):  
William M. Caton
2014 ◽  
Vol 22 (5) ◽  
pp. 5252 ◽  
Author(s):  
Christopher Matheisen ◽  
Michael Waldow ◽  
Bartos Chmielak ◽  
Simon Sawallich ◽  
Thorsten Wahlbrink ◽  
...  

Crystals ◽  
2020 ◽  
Vol 10 (10) ◽  
pp. 870
Author(s):  
Cheng-Kai Yang ◽  
Xu-Ping Wang ◽  
Fei Zhang ◽  
Hua-Di Zhang ◽  
Bing Liu ◽  
...  

KTa0.65Nb0.35O3 and Fe-doped KTa0.65Nb0.35O3 crystals were grown by the top-seeded solution growth method (TSSG). Fe ion doping significantly improves the electro-optic properties of cubic KTN crystals. We describe their electro-optic modulation theory and experimental research. The electro-optic modulation waveform deduced by theoretical calculation is basically consistent with the waveform measured in the experiment. We observed the attenuation of light modulation under multiple voltage cycles. The modulation curve of the crystal is inconsistent when the crystal voltage is boosting and bucking. Under the same voltage condition, the higher the incident light power, the faster the modulation depth attenuation. In this experiment, the size of the KTN crystal chip is 6 mm × 5 mm × 2 mm. We obtain the effective electro-optic coefficient as s11 − s12 = 1.34 × 10−15 m2/V2; the half-wave voltage near the Curie temperature is 39 V.


1985 ◽  
Vol 46 (3) ◽  
pp. 215-217 ◽  
Author(s):  
Demetri Psaltis ◽  
Hyuk Lee ◽  
Gabriel Sirat

Nature ◽  
1962 ◽  
Vol 193 (4818) ◽  
pp. 867-867 ◽  
Author(s):  
M. J. REDMAN ◽  
E. G. STEWARD

1985 ◽  
Vol 58 (12) ◽  
pp. 4666-4669 ◽  
Author(s):  
A. Hernández‐Cabrera ◽  
C. Tejedor ◽  
F. Meseguer
Keyword(s):  

2010 ◽  
Vol 25 (3) ◽  
pp. 253-257 ◽  
Author(s):  
E. J. Friedrich ◽  
R. Fernández-Ruiz ◽  
J. M. Merino ◽  
M. León

X-ray powder diffraction data for CuGa0.15In0.85Se2 and CuGa0.50In0.50Se2 are reported. Indexing of the X-ray diffraction powder pattern and the Rietveld refinement confirmed that these compounds crystallize in the tetragonal crystal system, with space group I-42d (No. 122) and lattice parameters of a=5.7528(2) Å and c=11.5225(3) Å for CuGa0.15In0.85Se2 and a=5.6847(1) Å and c=11.2817(1) Å for CuGa0.50In0.50Se2. The CuGaxIn1−xSe2 system presents the chalcopyrite type crystal structure (CuFeS2) and corresponds to two stacked zinc-blende unit cells. The metal atoms Cu, In, and Ga are regularly ordered in the unit cell. Every Se atom is tetrahedrally bonded to two Cu and two In and Ga atoms.


1994 ◽  
Author(s):  
Daumantas Ciplys ◽  
Romualdas Rimeika ◽  
Juozas Paskauskas

2010 ◽  
Vol 29-32 ◽  
pp. 1803-1808 ◽  
Author(s):  
Chun Li ◽  
Fan Yang ◽  
Wan Lin Guo

Strain-dependent electro-optic constant r33 and nonlinear optical coefficient d33 of ZnO are investigated systematically using density-functional theory based linear-response perturbation method. Miscellaneous properties, such as dielectric constants, elastic constants, piezoelectric coefficients, nonlinear optical coefficients, and electro-optic constants of other II-VI compound semiconductors (both Wurtzite and Zinc-blende structures) are also calculated for comparison with the results of unstrained ZnO. Extensive first-principles calculations show that both r33 and d33 of ZnO decrease almost linearly with increasing strains, which indicates that appropriate compression along the [0001] direction of ZnO could enhance its electro-optic and nonlinear optical properties, while stretching may weaken the corresponding properties. Among the involved Wurtzite structures, ZnO has the highest elastic constant, piezoelectric coefficient and electro-optic constant, showing practical importance.


Sign in / Sign up

Export Citation Format

Share Document