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    • 3. 发明专利
    • CRYSTAL SEALING CASE OF VARIABLE WAVELENGTH LASER DEVICE
    • JPS63133687A
    • 1988-06-06
    • JP28127086
    • 1986-11-26
    • HAMAMATSU PHOTONICS KK
    • URA TADAHISASUZUKI HIDEOOSUMI YASUTSUGUMORITA NOBUHIROMATSUMOTO OSAMUKOBAYASHI YUJIOBAYASHI YASUSHI
    • H01S3/108G02F1/39
    • PURPOSE:To prevent displacement of output laser beam position by changing an angle formed by the optical axis of laser beam and optical axis through formation of curved external surface of window for inputting or outputting laser beam of device including an arc centered to the intersecting point of the optical axis of nonlinear optical crystal and optical axis of laser beam. CONSTITUTION:A nonlinear optical crystal 11 and a case 12 for sealing the crystal 11 are formed integrally and wavelength of laser beam 25a emitted is changed by changing an angle formed by the optical axis 26 of laser beam 25 incident to the non-linear optical crystal 11 and optical axis of the nonlinear optical crystal 11. In this waveform variable laser device, the external circumference of windows 21, 22 for inputting and outputting laser beams 25, 25a of case 12 is formed as the curved surface including the arc centered at the intersecting point of the optical axis of nonlinear optical crystal 11 and optical axis 26 of laser beam 25. The external circumference of windows 21, 22 for inputting and outputting laser beams 25, 25a of the case 12 is formed, for example, in cylindrical having the center axis of the rotating axis 13 of case 12, or formed as the spherical surface centered on the intersecting point of the rotating axis 13 of case 12 and the optical axis 26 of the laser beam 25.
    • 5. 发明专利
    • OPTICAL PARAMETRIC OSCILLATOR
    • JPH01178938A
    • 1989-07-17
    • JP33371287
    • 1987-12-29
    • HAMAMATSU PHOTONICS KK
    • SUZUKI HIDEOOSUMI YASUTSUGUMORITA NOBUHIROMATSUMOTO OSAMUKOBAYASHI YUJIOBAYASHI YASUSHI
    • G02F1/39
    • PURPOSE:To vary the angle of the optical axis of exciting light to the optical axis of nonlinear optical crystal and to vary the output wavelength of oscillation light at a high speed by deflecting the exciting light by an optical deflector which utilizes the optoelastic effect of an optical material. CONSTITUTION:When specific electric power is supplied to the oscillator 13 of the optical deflector 10 and its oscillation frequency is varied within a specific range, the exciting light 5a changes its traveling direction and is deflected into exciting light 5b. Consequently, the light is reflected and converged by one focusing mirror 16, the angle ph of phase matching between the optical axis 19 of the exciting light 5b entering the nonlinear optical crystal 3 through an incidence mirror 14 and the optical axis 8 of the nonlinear optical crystal 3 varies, and the oscillation light 18 projected through a projection mirror 15 varies in wavelength corresponding to said variation. This utilizes the optoelastic effect of the optical material such as acoustooptic effect and electrooptic effect. Consequently, the deflecting speed of the exciting light 5a is increased to facilitate fast variation in the output wavelength of the oscillation light 18 and also eliminate the need for a crystal rotational mechanism.
    • 6. 发明专利
    • OPTICAL WAVELENGTH TUNABLE LASER APPARATUS
    • JPS63185084A
    • 1988-07-30
    • JP1754687
    • 1987-01-28
    • HAMAMATSU PHOTONICS KK
    • KOBAYASHI YUJIOBAYASHI YASUSHISUZUKI HIDEOOSUMI YASUTSUGUMORITA NOBUHIROMATSUMOTO OSAMU
    • H01S3/10G02F1/39H01S3/109
    • PURPOSE:To obtain an optical wavelength tunable laser without the large rotary angle of a crystal for an optical wavelength converter, by providing a second optical parametric oscillator having a specified function on the incident side of the optical wavelength converter. CONSTITUTION:When a crystal 6a for a first optical parametric oscillator (OPO) is excited with pumping lights, normal light and anomalous light are emitted when the angle (theta) of the crystal 6a is 90 degrees. Of the output light of the first OPO 1a, the pumping light is inputted into a 1/2 wavelength plate 27, and the direction of the polarized light is turned by 90 degrees. A crystal 6b for a second OPO 1b is provided at a position, which is orthogonally intersected with the crystal 6a for the first OPO. Therefore the pumping light becomes the normal light with respect to the crystal 6b for the second OPO. The phase is aligned with respect to the turning direction in a vertical plane. The signal light and the idler light, whose polarizing directions are orthogonally intersected with the output light of the first OPO 1a, are outputted. The output light from the first OPO 1a and the output light from the second OPO 1b are combined and inputted into an SHG 2. Then the normal light within a specified range with respect to a crystal 9 for the SHG is obtained. Said normal light becomes a wavelength tunable laser beam by the rotation of the crystal 9 for the SHG by 50-90 degrees.
    • 8. 发明专利
    • WAVELENGTH VARIABLE LASER DEVICE
    • JPS63159832A
    • 1988-07-02
    • JP31007386
    • 1986-12-24
    • HAMAMATSU PHOTONICS KK
    • SUZUKI HIDEOOSUMI YASUTSUGUMORITA NOBUHIROMATSUMOTO OSAMUKOBAYASHI YUJIOBAYASHI YASUSHI
    • H01S3/10G02F1/39H01S3/108
    • PURPOSE:To simultaneously output two laser beams of independent and variable wavelength by providing two optical parametric oscillators along the optical axis of an excitation light, and controlling the rotary angle of each non-linear optical crystal. CONSTITUTION:When a wavelength selecting signal is sent out to optical parametric oscillators 24, 25 through lines l1, l2 from a wavelength selecting circuit 45, the rotary angle of rotary shafts 30 and 32, and that of 40 and 42 are controlled to a prescribed angle respectively, and a phase matching angle of a non-linear optical crystal 31, and that of a non-linear optical crystal 41 are set to theta1 and theta2, respectively. Therefore, the oscillator 24 oscillates an optical parametric by the excitation light 22 of wavelength lambdap from a laser oscillator 21, and outputs the light beam 47 of lambda1s and lambda1i. Also, the oscillator 25 uses the transmission light of wavelength lambdap contained in the light beams 47, as an excitation light, executes a parametric oscillation through a collimator lens 37, and outputs the light beams 48 of wavelength lambda2s and lambda2i corresponding to the angle theta2. Also, in the output side of a filter 26, the light beams 49 of wavelength lambda1s and lambda2s appear simultaneously.