Patents Assigned to The Furukawa Electric Co., Ltd.
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Publication number: 20080260019Abstract: The burst oscillation device 20 includes the data generation part 21, the operation part 11, the signal selecting part 40 and the burst generation part 50. The generation part outputs the encoded data encoded based on data for communication. At the signal selecting part 40, the pulse release timing of predetermined repetition period is randomly delayed by the PPM and further delayed randomly by the minimal time by means of the PSK modulation, thereby realizing the decreasing of the peak value of the average power spectral density.Type: ApplicationFiled: June 13, 2008Publication date: October 23, 2008Applicant: The Furukawa Electric Co., Ltd.Inventor: Yasushi AOYAGI
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Publication number: 20080257072Abstract: [PROBLEMS] A (a) (b) separation unit can confirms a separation state, a detection unit enhances a lighting efficiency and a light reception sensitivity, and a dispensing unit ensures the normal state of a specimen. [MEANS FOR SOLVING PROBLEMS] A specimen separation device characterized by comprising a container for storing a specimen, a nozzle for sucking and ejecting the specimen from the container, a nozzle operating means for moving the nozzle vertically and laterally, and a nozzle controlling means for controlling the suction force and ejection force of the nozzle.Type: ApplicationFiled: April 25, 2005Publication date: October 23, 2008Applicant: The Furukawa Electric Co., Ltd.Inventors: Toru Takahashi, Ken Tsukii, Jie Xu
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Patent number: 7440167Abstract: An optical fiber for Raman amplification amplifies a signal light with a pumping light. A chromatic dispersion at a wavelength of 1,550 nm is in a range between ?70 ps/nm/km and ?30 ps/nm/km. Raman gain efficiency with a pumping light of 1,450 nm is equal to or more than 5 (W×km)?1. Nonlinear coefficient at the wavelength of 1,550 nm is equal to or less than 5.0×10?9 W?1. Zero-dispersion wavelength is neither at a wavelength of the signal light nor at a wavelength of the pumping light. Cut-off wavelength is equal to or less than the wavelength of the pumping light.Type: GrantFiled: June 22, 2007Date of Patent: October 21, 2008Assignee: The Furukawa Electric Co., Ltd.Inventors: Yuki Taniguchi, Yoshihiro Emori, Ryuichi Sugizaki, Atsushi Oguri, Takeshi Yagi
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Publication number: 20080254566Abstract: A surface-emitting semiconductor laser device includes a semi-insulating substrate, a layer structure with a bottom multilayer reflector, an n-type cladding layer, an active layer structure for emitting laser, a p-type cladding layer and a top multilayer reflector with a dielectric material, consecutively formed on the semi-insulating substrate, the active layer structure, the p-type cladding layer and the top multilayer reflector, configuring a mesa post formed on a portion of the n-type cladding layer, the p-type cladding layer or the p-type multilayer reflector. The surface-emitting semiconductor laser includes a p-side electrode formed on another portion of the p-type cladding layer, and an n-side electrode formed on another portion of the n-type cladding layer. The n-side electrode includes a substantially uniform Au film and AuGeNi film or AuGe film consecutively formed on the n-type cladding layer, and an alloy is formed between said Au film and said AuGeNi film or AuGe film.Type: ApplicationFiled: April 15, 2008Publication date: October 16, 2008Applicant: THE FURUKAWA ELECTRIC CO., LTD.Inventors: Noriyuki YOKOUCHI, Norihiro Iwai
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Publication number: 20080253716Abstract: An arrayed waveguide grating optical multiplexer/demultiplexer 1 comprises an arrayed waveguide grating 20 formed on a substrate 10. The arrayed waveguide grating 20 comprises two slab waveguides 21, 22, one arrayed waveguide 23, first input/output waveguides A, B respectively connected to each end facet 21a, 22a of slab waveguides 21, 22, and second input/output waveguide-groups C, D respectively connected to the end facets 21a, 22a. The first input/output waveguides A, B are provided for inputting or outputting a plurality of lights (?1˜?n) each of which has a different wavelength and multiplexed. The second input/output waveguides C, D are provided for individually inputting or outputting a plurality of lights (?1˜?n). One arrayed waveguide 23 can be used to carry out simultaneously multiplexing and demultiplexing. It is able to carry out simultaneously multiplexing and demultiplexing with one arrayed waveguide grating 20.Type: ApplicationFiled: March 27, 2008Publication date: October 16, 2008Applicant: The Furukawa Electric Co, Ltd.Inventor: Kazutaka Nara
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Patent number: 7431868Abstract: A metal substrate for an oxide superconducting wire, which comprises a polycrystalline metal substrate with a rolled aggregate structure having a {100} plane which is parallel to the rolled surface and a <001> axis which is parallel to the rolling direction, and an oxide crystal layer comprising an oxide of the polycrystalline metal and formed on a surface of the polycrystalline metal substrate, wherein at least 90% of grain boundaries in the oxide crystal layer have an inclination of 10° or less, and at least 90% of the {100} plane of the oxide crystal layer make an angle of 10° or less with the surface of the polycrystalline metal substrate.Type: GrantFiled: September 30, 2005Date of Patent: October 7, 2008Assignees: The Furukawa Electric Co., Ltd., International Superconductivity Technology Center, Sumitomo Electric Industries Ltd.Inventors: Toshihiko Maeda, Toru Izumi, Katsuya Hasegawa, Shigenobu Asada, Teruo Izumi, Yuh Shiohara
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Publication number: 20080243405Abstract: In the method for estimating battery residual capacity of the present invention, the voltage measurement values are obtained (step S2). And once it is finished, using the initial values of the coefficients set at the step S3 as starting, the optimization is progressed with renewing each value of the coefficients on the following iterating calculations (step S4). Once the optimum value of each coefficient in the approximation is determined at the step S4, the stable open circuit voltage is calculated by the optimized reciprocal function using thereof at the step S5. And then based thereon, the battery residual capacity is calculated by the predetermined conversion method (step S6).Type: ApplicationFiled: March 4, 2008Publication date: October 2, 2008Applicant: THE FURUKAWA ELECTRIC CO., LTDInventor: Noriyasu IWANE
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Publication number: 20080239465Abstract: In a method of phase adjustment for the demodulator 1 of the present invention, the phase adjustment is performed by driving any one of the heaters on the two waveguides 10 and 11 in the Mach-Zehnder interferometer (MZI) 6 and on the two waveguides 14 and 15 in the MZI 7. In case that an initial phase difference between the MZIs 6 and 7 smaller than a required phase difference as ?/2 therebetween, the heaters C and D are driven, that are formed on the first waveguide 10 in the MZI 6, and the heaters G and H are driven, that are formed on the second waveguide 15 in the MZI 7. In case that the initial phase difference is larger than the required phase difference (?/2) therebetween, the heaters A and B formed on the second waveguide 11 in the MZI 6, and the heaters E and F formed on the first waveguide 14 in the MZI 7 are driven.Type: ApplicationFiled: March 5, 2008Publication date: October 2, 2008Applicant: The Furukawa Electric Co., Ltd.Inventors: Junichi Hasegawa, Kazutaka Nara
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Publication number: 20080240727Abstract: The tunable dispersion compensator 10 of the present invention comprises: the Mach-Zehnder interferometers (MZIs) 21 to 25 cascaded on a planar lightwave circuit; and the tunable couplers 31 to 34 connected to between each corresponding pair of the MZIs respectively. The Y-branch waveguide 15 and 16 are used for connecting to between the MZIs 21, 25 as both end sides and the input/output optical waveguides 13, 14 respectively. The waveguide loop mirror 40 is connected to the final stage MZI 25 among the MZIs 21 to 25 which an incident light is propagated last therethrough. The half-wave plate 50 is inserted to the loop waveguide 41 of the waveguide loop mirror 40. And it becomes able to enhance (double) the amount of tunable dispersion because an input light signal is passed twice through the similar path by the waveguide loop mirror 40.Type: ApplicationFiled: March 5, 2008Publication date: October 2, 2008Applicant: The Furukawa Electric Co., Ltd.Inventors: Hiroshi Kawashima, Kazutaka Nara
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Publication number: 20080240645Abstract: An optical integrated circuit 1 according to the present invention includes a planar lightwave circuit 2, and a semiconductor element 3, which are fixed at one contact surface 12. A semiconductor optical amplifier (SOA) 9 is formed on a semiconductor substrate 8. A semiconductor waveguide 10 and a semiconductor waveguide 11 are formed on an input side and an output side of SOA 9, respectively. The semiconductor waveguide 11 has a turnaround portion 11a turned around on the semiconductor substrate 8. Respective ends of the optical waveguides 5 and 6 on a PLC platform 4 and respective ends of semiconductor waveguides 10 and 11 are optically coupled with each other at the contact surface 12.Type: ApplicationFiled: March 10, 2008Publication date: October 2, 2008Applicant: THE FURUKAWA ELECTRIC CO., LTD.Inventors: Masaki FUNABASHI, Junichi Hasegawa, Takeshi Akutsu, Kazutaka Nara, Noriyuki Yokouchi
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Publication number: 20080240192Abstract: A surface emitting laser element includes an active layer and a dielectric multilayer mirror formed with a plurality of dielectric layers having different refractive indices for reflecting a light generated in the active layer. At least one of boundaries between the dielectric layers is formed to have a predetermined surface roughness to obtain a desired target reflectance of the dielectric multilayer mirror.Type: ApplicationFiled: March 28, 2008Publication date: October 2, 2008Applicant: The Furukawa Electric Co, Ltd.Inventors: Takeo KAGEYAMA, Norihiro Iwai, Yasumasa Kawakita, Keishi Takaki, Peter Nyakas
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Publication number: 20080232750Abstract: An optical fiber ribbon includes a plurality of optical fibers, each includes a glass optical fiber coated with a fiber coating, that are arranged in parallel, and a ribbon coating that coats the optical fibers arranged in parallel. The optical fiber ribbon has a thickness equal to 300 ?m or less. The fiber coating is made of a non-flame-resistant ultraviolet curable resin. The ribbon coating has a thickness equal to 40 ?m or more and is made of a flame resistant resin.Type: ApplicationFiled: May 6, 2008Publication date: September 25, 2008Applicant: THE FURUKAWA ELECTRIC CO., LTD.Inventors: Harumi Inaba, Ryuichi Sugizaki, Takeshi Yagi
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Publication number: 20080225276Abstract: A method of simultaneously specifying the wavelength dispersion and nonlinear coefficient of an optical fiber. Pulsed probe light and pulsed pump light are first caused to enter an optical fiber to be measured. Then, the power oscillation of the back-scattered light of the probe light or idler light generated within the optical fiber is measured. Next, the instantaneous frequency of the measured power oscillation is obtained, and the dependency of the instantaneous frequency relative to the power oscillation of the pump light in a longitudinal direction of the optical fiber is obtained. Thereafter, a rate of change in the longitudinal direction between phase-mismatching conditions and nonlinear coefficient of the optical fiber is obtained from the dependency of the instantaneous frequency. And based on the rate of change, the longitudinal wavelength-dispersion distribution and longitudinal nonlinear-coefficient distribution of the optical fiber are simultaneously specified.Type: ApplicationFiled: February 12, 2008Publication date: September 18, 2008Applicant: The Furukawa Electric Co., Ltd.Inventors: Masateru Tadakuma, Yu Mimura, Misao Sakano, Osamu Aso, Takeshi Nakajima, Katsutoshi Takahashi
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Publication number: 20080226246Abstract: An optical fiber transmits at least a signal light having a wavelength of 1550 nanometers in a fundamental propagation mode. The optical fiber has, a cutoff wavelength equal to or longer than 1550 nanometers, a wavelength dispersion of 4 ps/nm/km to 7 ps/nm/km in the fundamental propagation mode at the wavelength of 1550 nanometers, a dispersion slope of a positive value equal to or smaller than 0.03 ps/nm2/km in the fundamental propagation mode at the wavelength of 1550 nanometers, an effective core area equal to or larger then 60 ?m2 in the fundamental propagation mode at the wavelength of 1550 nanometers, and a bending loss equal to or smaller than 20 dB/m with a winding of 16 turns at a diameter of 20 millimeters in the fundamental propagation mode at the wavelength of 1550 nanometers.Type: ApplicationFiled: March 11, 2008Publication date: September 18, 2008Applicant: The Furukawa Electric Co., Ltd.Inventor: Katsunori IMAMURA
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Publication number: 20080226241Abstract: An optical fiber, made of silica-based glass, comprising a core and a cladding. The optical fiber having a mode field diameter of 6.5 ?m or larger at a wavelength of 1300 nm, transmitting light with a wavelength of 1250 nm in a single mode, and having a bending loss of 1 dB/turn or smaller at a wavelength of 1300 nm when the optical fiber is bent with a curvature radius of 1.5 mm.Type: ApplicationFiled: May 21, 2008Publication date: September 18, 2008Applicant: The Furukawa Electric Co., Ltd.Inventors: Ryuichi SUGIZAKI, Iwao SHIMOTAKAHARA, Harumi INABA, Takeshi YAGI
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Patent number: 7426027Abstract: A small object identifying device and its identifying method according to which a large number of small objects can be identified. In one embodiment, the device includes a dispersion region section which disperses a large quantity of several kinds of small objects which are labeled by a combination of the presence/absence or measure of label elements of several kinds. A measuring device distributes and associates kinds of said label elements to two or more measurement points and measures the presence/absence or the measure of said label elements of the kinds which have been associated with respective measurement points. An identifying section associates the measurement results measured at each measurement point to thereby identify said small objects.Type: GrantFiled: October 4, 2007Date of Patent: September 16, 2008Assignees: Precision Systems Science Co., Ltd., The Furukawa Electric Co., Ltd., Fi-Techno Co., Ltd.Inventors: Masahisa Noguchi, Ken Tsukii, Hideji Tajima
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Publication number: 20080216516Abstract: A coating is applied on an optical fiber drawn from a melted tip of an optical-fiber preform. A glass spin is applied to a coated optical fiber by gripping the coated optical fiber with at least a pair of spinning applying rollers arranged in different levels with parallel rotation axes, rotating the spinning applying rollers so that the coated optical fiber is guided in a predetermined direction, and alternately shifting the spinning applying rollers in opposite directions along the rotation axes. The glass spin is applied to the coated optical fiber in a state in which each of the rotation axes is tilted at a predetermined angle from a plane perpendicular to the first direction.Type: ApplicationFiled: February 29, 2008Publication date: September 11, 2008Applicant: THE FURUKAWA ELECTRIC CO., LTD.Inventors: Minsuk Song, Shinichi Arai
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Publication number: 20080219667Abstract: With this scheme, there is provided an optical communication system and a dispersion-compensating optical fiber with which a long-haul optical signal transmission is possible by making use of the low optical nonlinearity and the low transmission loss characteristic of the photonic bandgap optical fiber.Type: ApplicationFiled: April 23, 2008Publication date: September 11, 2008Applicant: The Furukawa Electric Co, Ltd.Inventor: Katsunori IMAMURA
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Patent number: 7424191Abstract: A method of simultaneously specifying the wavelength dispersion and nonlinear coefficient of an optical fiber. Pulsed probe light and pulsed pump light are first caused to enter an optical fiber to be measured. Then, the power oscillation of the back-scattered light of the probe light or idler light generated within the optical fiber is measured. Next, the instantaneous frequency of the measured power oscillation is obtained, and the dependency of the instantaneous frequency relative to the power oscillation of the pump light in a longitudinal direction of the optical fiber is obtained. Thereafter, a rate of change in the longitudinal direction between phase-mismatching conditions and nonlinear coefficient of the optical fiber is obtained from the dependency of the instantaneous frequency. And based on the rate of change, the longitudinal wavelength-dispersion distribution and longitudinal nonlinear-coefficient distribution of the optical fiber are simultaneously specified.Type: GrantFiled: October 13, 2006Date of Patent: September 9, 2008Assignee: The Furukawa Electric Co., Ltd.Inventors: Masateru Tadakuma, Yu Mimura, Misao Sakano, Osamu Aso, Takeshi Nakajima, Katsutoshi Takahashi
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Publication number: 20080212925Abstract: The present invention provides an optical fiber for a fiber Bragg grating having a high reliability and superior performance. An optical fiber according to the present invention has a glass film containing micro porous bodies formed on the circumference of the optical fiber having a photosensitive core or both of the photosensitive core and a cladding.Type: ApplicationFiled: December 26, 2007Publication date: September 4, 2008Applicant: THE FURUKAWA ELECTRIC CO., LTD.Inventors: Yoshihiro ARASHITANI, Kazuhiko Kashima, Yasuo Uemura, Mitsunori Okada