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Compact and high reliable blue coherent light sources are required for the optical data storage of high density, color image processing and optical measurements.One of the possible approaches is the direct frequency doubling of the near infrared semiconductor laser by optical waveguide techniques. So a material applied to the second harmonic generation (SHG) must not only have high molecular hyperpolarizability (β) but also have complete transparency at both the fundamental
Compact and high reliable blue coherent light sources are required for the optical data storage of high density, color image processing and optical measurements. One of the possible approaches is the direct frequency doubling of the near infrared semiconductor laser by optical waveguide techniques. So a material applied to the second harmonic generation (SHG) must not only have high molecular hyperpolarizability (β) but also have complete transparency at both the fundamental