Optical harmonic generator

Electrical transmission or interconnection systems – Nonlinear reactor systems – Multiaperture

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372 22, 350388, 350392, G02F 135

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active

045104026

ABSTRACT:
A pair of uniaxial birefringent crystal elements are fixed together to form a serially arranged, integral assembly which, alternatively, provides either a linearly or elliptically polarized second-harmonic output wave or a linearly polarized third-harmonic output wave. The "extraordinary" or "e" directions of the crystal elements are oriented in the integral assembly to be in quadrature (90.degree.). For a second-harmonic generation in the Type-II-Type-II angle tuned case, the input fundamental wave has equal amplitude "o" and "e" components. For a third-harmonic generation, the input fundamental wave has "o" and "e" components whose amplitudes are in a ratio of 2:1 ("o":"e" reference first crystal). In the typical case of a linearly polarized input fundamental wave this can be accomplished by simply rotating the crystal assembly about the input beam direction by 10.degree.. For both second and third harmonic generation input precise phase-matching is achieved by tilting the crystal assembly about its two sensitive axes ("o").

REFERENCES:
patent: 3387204 (1968-06-01), Ashkin et al.
patent: 3741626 (1973-06-01), Wentz
Craxton, "Theory of High Efficiency . . . Radiation", Optics Communication, vol. 34, No. 3, Sep. 1980, pp. 474-478.
Seka et al., "Demonstration of High Efficency . . . Radiation", Optics Communication, vol. 34, No. 3, Sep. 1980, pp. 469-473.
Summers et al., "A Two Color . . . Lasers", Lawrence Livermore Laboratory Technical Information Sheet, Jan. 12, 1981.
Summers et al., "Nova Frequency Conversion System", Oct., 1981.

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