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    • 2. 发明专利
    • OPTICAL FREQUENCY MULTIPLEX SIGNAL PROCESSING METHOD
    • JPH04134726A
    • 1992-05-08
    • JP25933190
    • 1990-09-26
    • MITSUBISHI ELECTRIC CORP
    • YAGYU EIJINISHIMURA TETSUYAYOSHIMURA MOTOMUTSUKADA NORIAKI
    • G11B7/00G11B7/0045G11B7/005
    • PURPOSE:To allow the higher speed optical frequency multiplex signal processing of frequency region by shifting the absorption spectra of the light of a medium which changes the absorption spectra by an optical Start effect. CONSTITUTION:The optical Stark effect is generated in a memory region 51 and the absorption spectra of the light of the memory region 51 are shifted to the high frequency side according to the intensity of a laser beam 7 for stimulation when the laser light 7 for stimulation of the frequency omegaP from the laser 1 for stimulation is deflected by an optical deflector 4 and is made incident on the memory region 51 of an optical recording medium 5. Then, the shift arises in the absorption spectra of the light of the medium 5 and, therefore, the frequency multiplex incident light is eventually subjected to the intensity modulation in the frequency region and the frequency multiplex exit light subjected to the intensity modulation in the frequency region is obtd. The signal multiplexed in the frequency region is reproduced at a high speed from the optical recording medium in this way without subjecting the light for signal reproduction to frequency scanning and the signal processing to the arbitrary frequency multiplex incident light is possible.
    • 4. 发明专利
    • OPTICAL FUNCTIONAL DEVICE
    • JPH02309327A
    • 1990-12-25
    • JP13213489
    • 1989-05-24
    • MITSUBISHI ELECTRIC CORP
    • TSUKADA NORIAKITOKUDA YASUKI
    • G02F1/35G02F3/02
    • PURPOSE:To obtain an optical functional device capable of realizing an optical memory element, an optical logical element and an optical switching element. etc., which use the wavelength of light as information amount by combining an optical bistable element having (p-i-n) structure for making quantum well structure function as a light absorption part with a wavelength variable laser. CONSTITUTION:The optical bistable element 20a in which the intensity of light of output is set so as to show bistability for a certain wavelength region of the light has the (p-i-n) structure for making the quantum well structure function as the light absorption part and is set so that the intensity of outgoing light may show bistability or hysteresis characteristic within the specified range of the light absorption quantity in the light absorption part. When the bistable element 20a is irradiated with the light from the wavelength variable laser element 30, the intensity of the output light becomes stable for a certain wavelength region of the light. By changing the wavelength over the wavelength region, the intensity of the output light is settled at another stable point in terms of bistability. Namely, the optical memory element, the optical logical element and the optical switching element, etc., where the processing of information can be performed by setting the wavelength of incident light as a medium can be constituted, and the wavelength is utilized for processing optical information in addition to the intensity of the light.
    • 6. 发明专利
    • OPTICAL NONLINEAR ELEMENT
    • JPH0287125A
    • 1990-03-28
    • JP23941688
    • 1988-09-22
    • MITSUBISHI ELECTRIC CORP
    • TOKUDA YASUKITSUKADA NORIAKI
    • G02F1/35G02F1/017
    • PURPOSE:To vary the absorption characteristics according to the wavelength of signal light by flattening the bend of the energy band in a light absorption region by the carrier formed by incidence of the signal light. CONSTITUTION:A quantum well layer 25 of 100Angstrom and a quantum well layer 26 of 80Angstrom are laminated via a tunnel barrier layer 27 to constitute an asymmetric bond quantum well structure. The band structure is bent in the thermally equil. state because of the built-in electric field and is flattened because of screening by photoexcitation carriers when the intensity of the incident light is gradually increased. Since the carriers generated by the photoexcitation in such a manner negate the built-in electric field made in a p-i-n junction, the energy band is nearly flattened and the quantum levels are intersected at this time, by which the absorption peak wavelength is changed. The absorption characteristics are varied in this way according to the wavelength.
    • 10. 发明专利
    • WAVELENGTH-TUNABLE SEMICONDUCTOR LASER DEVICE
    • JPS63281491A
    • 1988-11-17
    • JP11740387
    • 1987-05-13
    • MITSUBISHI ELECTRIC CORP
    • TSUKADA NORIAKIFUJIWARA KENZOTOKUDA YASUKI
    • H01S5/00H01S5/026H01S5/0625H01S5/10H01S5/34
    • PURPOSE:To enlarge the variable range of a laser oscillation wavelength, and increase the response speed, by shifting the exceton energy level of the quantum well active layer of a first semiconductor laser to the higher energy side, by the laser beam of a second semiconductor laser, whose wavelength is shorter than the oscillation wavelength of a first semiconductor laser. CONSTITUTION:A DFB laser A and a DH laser B are formed on the same substrate 1. (2) is an n-AlGaAs lower clad layer. (21) is a laser active layer composed of a multi-quantum well structure of a GaAs layer and an AlGaAs layer. (4) is a p-AlGaAs upper clad layer. (5) is a p GaAs cap layer. (6) and (6b) are upper surface electrodes. (6c) is a lower rear electrode. (7) is a diffraction grating region of the DFB laser A. A band end portion exists in the semiconductor. A light having a wavelength longer than it can be transmitted, and a light having a wavelength shorter than it is absorbed in the semiconductor surface. When a laser light is turned on in the state where the wavelength omegaof an emitted laser beam is separated toward the long wavelength side from the absorption peak omega0(omega0>omega), the absorption spectrum of excitation can be shifted to the short wavelength side by the AC Stark effect.