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    • 56. 发明专利
    • LIGHT MODULATION DEVICE AND CONOSCOPIC HOLOGRAPHY-SYSTEM
    • JPH0728100A
    • 1995-01-31
    • JP21167791
    • 1991-07-29
    • CENTRE NAT ETD TELECOMM
    • AHARON AGURANATOGABURIERU SHIRAATO
    • G02F1/17G02F1/01G02F1/21G03C1/725G03H1/06
    • PURPOSE: To realize removal of a continuous wave component and control of an optimum transmittance while keeping the dynamic range of light to be transmitted by providing a crystal in the cavity part of an interference system having a transmittance-optical distance characteristic and applying an external electric field to the crystal. CONSTITUTION: Crystal 1 having a refracting property is arranged in an optical cavity part of an interferometer system 2 which has an inclination to lead a dynamic range where the transmittance is most changed for the least change of the refractive index. The range of the cavity part is determined by semitransparent mirrors 21 and 22. When write-in light qe is made incident, it is absorbed by the refractive index of crystal 1, and when a read light q1 is made incident next, the transmittance characteristic of the interferometer 2 is changed because the refractive index of crystal 1 is changed by the write-in light qe already made incident. Further, the optimum transmittance is controlled to a desired value by the electric field with can control the refractive index of crystal. Consequently, the dynamic range is increase in accordance with the inclination of the transmittance-optical distance characteristic.
    • 57. 发明专利
    • FULLY OPTICAL ELEMENT
    • JPH0720510A
    • 1995-01-24
    • JP16445593
    • 1993-07-02
    • NEC CORP
    • TAJIMA KAZUTO
    • G02F1/21G02F1/225G02F1/313G02F1/35G02F3/00
    • PURPOSE:To provide the Mach-Zehnder type fully optical element with which the switch off time does not depend on the relaxation time of a nonlinear effect by introducing control light into respective optical nonlinearity developing parts of both arms of a Mach-Zehnder system. CONSTITUTION:This fully optical element has control light input ports A, B at both arms A, B of the Mach-Zehnder system. The control light B changes the refractive index of the nonlinear waveguide B by photoexciting the nonlinear waveguide B of the arm B. The control light A excites the arm A 50ps after excitation by the control light B. The pulse energy of the control light A is the extent of exiting the carriers remaining in the nonlinear waveguide B at the moment the control light A excites the nonlinear waveguide A and is weaker than the control light B. The effective lengths of both arms A, B are, therefore, made into the same at the moment the control light A excites the nonlinear waveguide A. Then, the output light thereof rapidly rises (switch on) at the excitation of the control light B and rapidly restores the original state (switch off) at the moment of the excitation of the control light A.