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    • 4. 发明专利
    • WAVEGUIDE TYPE OPTICAL CIRCUIT AND ITS PRODUCTION
    • JPH1039150A
    • 1998-02-13
    • JP19442096
    • 1996-07-24
    • NIPPON TELEGRAPH & TELEPHONE
    • TAKAHASHI HIROSHIHIMENO AKIRA
    • G02B6/122G02B6/13
    • PROBLEM TO BE SOLVED: To lessen the dependence on temp. by forming a layer having a coefft. of thermal expansion different from the coefft. of thermal expansion of a substrate. SOLUTION: The waveguide type optical circuit 2 includes at least a silicon substrate 1 and a plane type optical waveguide formed on the substrate 1. The layer having a coefft. of thermal expansion different from the coefft. of thermal expansion of the substrate 1 is formed on the lower side of the substrate 1 or the upper side of the plane type optical waveguide or both thereof. For example, the circuit is constituted by adhering a titanium-added quartz glass plate 3 which is the layer having the coefft. of thermal expansion different from the coefft. of thermal expansion of the substrate 1 on the upper side of the substrate 1 to suppress the expansion and contraction of the silicon substrate 1. At the time of manufacture, a quartz glass film is formed on the silicon substrate 1 by using a flame hydrolysis glass film deposition method and executing patterning of the waveguides by photolithography and reactive ion etching. The titanium-added quartz glass plate 3 is thereafter adhered as a low αplate by using an epoxy adhesive. Further preferably, the layer having the coefft. of thermal expansion smaller than the coefft. of thermal expansion of the substrate 1 is formed on the lower side of the substrate 1 or the upper side of the plane type optical waveguide or both thereof.
    • 5. 发明专利
    • ARRAY WAVEGUIDE TYPE OPTICAL MULTIPLEXER/DEMULTIPLEXER
    • JPH08334637A
    • 1996-12-17
    • JP14015295
    • 1995-06-07
    • NIPPON TELEGRAPH & TELEPHONE
    • TAKAHASHI HIROSHIINOUE YASUYUKI
    • G02B6/12
    • PURPOSE: To stably obtain an array waveguide type optical multiplexer/ demultiplexer which is free from reflected return light by imparting a slight inclination to the direction of the groove disposed near a straight line connecting the mid-points of waveguides. CONSTITUTION: The groove 7 crossing the waveguides constituting array waveguide diffraction gratings 4(9)s cut at the canter of the array waveguide diffraction gratings 4 in order to eliminate the dependency on polarization. The groove 7 is not perpendicular to the waveguides constituting the array waveguide diffraction gratings 4 but inclines slightly with a horizontal direction. The array waveguide diffraction gratings 4 are so constituted that δθ meets the equation when the spacing of the input waveguides 2 in the juncture to a first slab waveguide 3 is defined as Δx, the radius of curvature of the first slag waveguide 3 as (f), the spacing of the plural waveguides varying in lengths in the parts intersecting with the groove as D, the effective refractive index of the slag waveguide 3 as ns , the effective refractive index of the plural waveguides varying in the lengths as nc and the angle formed by the groove 7 and the plural waveguides varying in the lengths as x/2±δθ(radian).
    • 6. 发明专利
    • CIRCULAR WAVEGUIDE TM11 MODE FILTER
    • JPH08204401A
    • 1996-08-09
    • JP878295
    • 1995-01-24
    • SHIMADA PHYSICAL CHEM IND CONIPPON TELEGRAPH & TELEPHONE
    • ASARI SATORUKONDO AKIRAHIGA HIDEMITSUMORIKAWA YOFUMITAKAHASHI HIROSHI
    • H01P1/16H01P1/30
    • PURPOSE: To diffuse heat generated in a resistor bar on the wall surface of a circular waveguide satisfactorily by arranging plural cruciform dielectrics of thickness thinner than guide wave length in the circular waveguide and supporting the resistor bar with their arm parts. CONSTITUTION: Two cruciform dielectrics 7 of thickness sufficiently thinner than the wave guide length of the circular waveguide 1 and of diameter nearly equal to that of the circular waveguide 1 and with high thermal conductivity and low dielectric constant are arranged in the circular waveguide 1 keeping a prescribed interval. Such interval between the cruciform dielectrics 7 can be selected at a distance so as to negate mutual impedance non-matching in a required frequency area. Each of the arm parts 7a-7d of the cruciform dielectrics 7 is formed in such a way that a hole of same diameter as that of the resistor bar 3 is opened at a position in which an electric field in the cross-sectional direction of a circular TM mode is mostly concentrated advancing the direction of tubal axis, and the resistor bar 3 is inserted through the hole, and supported by adhering with a conductive adhesive. Therefore, the heat generated in each resistor bar 3 is propagated through the cruciform dielectric 7 and diffused on the circular waveguide 1, which suppresses temperature rise in each resistor bar 3.
    • 8. 发明专利
    • WAVEGUIDE TYPE OPTICAL COUPLER
    • JPH04163406A
    • 1992-06-09
    • JP28938090
    • 1990-10-26
    • NIPPON TELEGRAPH & TELEPHONE
    • TAKAHASHI HIROSHINISHI NORIOOKUNO MASAYUKI
    • G02B6/12G02B5/18G02B6/34
    • PURPOSE:To eliminate the polarization dependence without necessity of eliminating double refraction of respective channel waveguides by arranging a polarization separation circuit and two input waveguides for horizontal polarized light and for vertical polarized light. CONSTITUTION:The wavelength multiple signal light from a transmission line 9 are separated into a horizontal polarization (TE) light component and a vertical polarization (TM) light component by means of a polarization separation circuit 10, and through polarization holding fibers 11, 12 the TE polarization light component and the TM polarization light component pass through the first input waveguide 2 and the second input waveguide 3 respectively, leading to incidence on an input side slab waveguide 4. The light diffuses because no horizontal confinement exists within the slab waveguide, and waves are guided into a plurality of channel waveguide 6. After receiving the required phase difference at an array waveguide, the light is emitted to the output side slab waveguide, and converges in the vicinity of the center of curvature. The converging position is obtained from a different output waveguide 8 based on the wavelength according to the phase difference received at the array waveguide.