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Linear Electro-optic Effect of 0.88Pb(Zn<sub>1/3</sub>Nb<sub>2/3</sub>)O<sub>3</sub>–0.12PbTiO<sub>3</sub> Single Crystal
71
Citations
12
References
2000
Year
Materials ScienceRoom TemperatureOptical MaterialsDielectric ConstantEngineeringPhysicsCrystal MaterialOptical PropertiesPoled 0.88PbOptical TestingApplied PhysicsQuantum MaterialsCrystalsLinear Electro-optic EffectOptoelectronicsElectro-optics Device
The linear electro-optic (E-O) coefficients of poled 0.88Pb(Zn 1/3 Nb 2/3 )O 3 –0.12PbTiO 3 single crystal were characterized using an automated scanning Mach-Zehnder interferometer and the senarmont compensator method at room temperature. They were obtained at a wavelength of 632.8 nm: r 33 =134 pm/V, r 13 =7 pm/V, r 51 =462 pm/V, and r c =131 pm/V respectively and the refractive indices: n e =2.57 and n o =2.46. The large r 51 coefficient compared with r 33 is caused by the high dielectric constant at perpendicular to the polar-axis compared with the dielectric constant along the c -axis. Comparison with the quadratic E-O coefficients measured at near and above the Curie temperature suggests that the values of the quadratic E-O coefficients measured earlier may be smaller than the intrinsic ones due to the influence of micro-polar regions. The development of an automated scanning Mach-Zehnder interferometer, which is less susceptible to the errors caused by the laser intensity fluctuation and drafting in the optical path length in the system, is also described.
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