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    • 43. 发明专利
    • PREPARATION FOR ROUND LIGHT WAVEGUIDE LINE
    • JPS56126808A
    • 1981-10-05
    • JP2915180
    • 1980-03-10
    • NIPPON TELEGRAPH & TELEPHONE
    • MURAKAMI TAIJIIKEDA MASAHIRO
    • G02B6/13G02B6/30
    • PURPOSE:To reduce a connection loss to a cyindrical optical fiber, by making round the sectional form of a light waveguide line. CONSTITUTION:A glass layer of a high refractive index, having a lower softening temperature than that of the substrate 6 is formed on the substrate made of a light resisting material. A waveguide line having a rectangular section is formed by performing, for instance, the reactive spatter etching treatment. Subsequently, the whole substrate 6 on which the rectangular waveguide line has been formed is retained for a few minutes at a temperature which is lower than a softening temperature which is lower than a softening temperature of the substrate, and also higher than a softening temperature of glass forming the waveguide line. As a result, the waveguide line is shaped to a waveguide line 10 having a round section, by means of surface tension of said glass. The waveguide line is embedded by use of a glass layer which has a lower softening temperature than that of glass forming the waveguide 10, and has a lower refractive index than that of said glass. Subsequently, it is made a transparent glass layer 12 by heating to 1,000-1,200 deg.C.
    • 45. 发明专利
    • VARIABLE TYPE PHOTO DIRECTIONAL COUPLER
    • JPS5640808A
    • 1981-04-17
    • JP11612279
    • 1979-09-12
    • NIPPON TELEGRAPH & TELEPHONE
    • MURAKAMI TAIJIMIKAMI OSAMUIZAWA TATSUO
    • G02B6/12G02F1/11G02F1/335
    • PURPOSE:To make manufacture easy by parallel disposing the two optical waveguides comprising transparent dielectric or liquid of a refractive index higher than that of the circumference within a substrate so that ultrasonic waves may be propagated in the optical waveguides and changing the propagation constants of the optical waveguides by ultrasonic waves thereby changing the coupling constant thereof. CONSTITUTION:Optical waveguides 2, 2' of transparent dielectric or CCl4 of a refractive index higther than that of the circumference are formed within a substrate 1 of glass or the like. These optical waveguides 2, 2' have parallel parts 2A and 2A' of a length l. An ultrasonic transducer 3, an electrode 5 and a reflecting plate 6 are provided to the substrates and ultrasonic waves are generated with a high- frequency electric power source 4. The light 7 incident to one waveguide 2 couples 100% in the parallel parts 2A, 2A' and is taken out as exit light 8 from the waveguide 2'. If the ultrasonic waves are generated and the inter-axis distance between the waveguides 2 and 2' is set at a half wavelength, a propagation constant difference is produced in the two optical guides 2, 2', and this makes the intensity of the exit rays 8 and 9 variable. Thereby, the manufacture of the variable couplers of low losses can be made easy.
    • 46. 发明专利
    • OPTICAL FILTER
    • JPS5478144A
    • 1979-06-22
    • JP14518277
    • 1977-12-05
    • NIPPON TELEGRAPH & TELEPHONE
    • MURAKAMI TAIJITSUCHIYA HARUHIKO
    • G02B6/00G02B6/28G02B6/293G02B6/34
    • PURPOSE:To eliminate the need for optical axis adjustment and provide a small filter of sharp rise by making use of the optical loss of a single mode waveguide of different radii of curvature or multiple waveguides of the same radius of curvature. CONSTITUTION:The incident light to a single mode optical guide 1 with an external layer is bisected to the guide light by the core part 4 and the radiation light reflecting at the boundary 6 with the external layer of the clad 5 of a refractive index n2 smaller than that of the core part 4 and a half-amplitude level (b) by the bent parts whose radii of curvature R1 thru R3 become subsequently smaller. When the conditions of the formulas I, II wherein the phase difference of the radiation light and guide mode becomes N(integer) times of 2pi are satisfied, coupling of the radiation light and guide light becomes maximum and the guide light is converted to the radiation light, which is then radiated to the outside from the reflection point of the boundary 6, thus the light loss of the guide light becomes large. (In the formulas beta : the phase constant of the guide mode, K : the number of light waves of free space)