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    • 5. 发明专利
    • BROAD-BAND HIGH-SPEED WAVELENGTH CONVERSION METHOD AND DEVICE THEREFOR
    • JPH10325970A
    • 1998-12-08
    • JP20729597
    • 1997-07-16
    • RIKAGAKU KENKYUSHO
    • AKAGAWA KAZUYUKIWADA TOMOYUKITASHIRO HIDEO
    • G02F1/37H01S3/109
    • PROBLEM TO BE SOLVED: To enable the alignment to a phase matching angle with respect to a laser beam and to enable high-speed higher modulation conversion without rotating a nonlinear optical crystal by controlling the incident angle of the laser beam made incident on the nonlinear optical crystal according to the dispersion characteristics of a dispersion element and the condensing characteristics of a condenser element. SOLUTION: The exciting laser beam is refracted in the optical path according to the wavelength by a first prism 12 which is the dispersion element, by which the optical path of the beam is divided by each wavelength of the exciting laser beam. The incident angle on the nonlinear optical crystal 10 is adjusted so as to be optimized at respective wavelengths by a first cylindrical concave surface mirror 14 which is the condenser element. On the other hand, the converted laser beam emitted from the nonlinear optical crystal 10 is adjusted in the optical path and is made incident on a second prism 18 by a second cylindrical concave surface mirror 16 which is the condenser element. The laser beam is refracted and is emitted through a prescribed optical path. The alignment of the nonlinear optical crystal 10 to the phase matching angle with respect to the incident laser beam is made possible without rotating the nonlinear optical crystal according to this wavelength conversion method.
    • 6. 发明专利
    • LASER WAVELENGTH CONVERTER
    • JPH1039347A
    • 1998-02-13
    • JP21194696
    • 1996-07-23
    • RIKAGAKU KENKYUSHO
    • TASHIRO HIDEOTSUNEMI AKIRASAITO TOKUHITONAGASAKA KEIGO
    • G02F1/35H01S3/106H01S3/30
    • PROBLEM TO BE SOLVED: To make it possible to attain high Raman conversion efficiency without the increase in size and complication by making the optical axis of the light passing a first resonator back and forth and the optical axis of the light passing a second resonator back and forth coaxial. SOLUTION: The exciting laser beam resonator 16 comprises a reflection mirror 12 for reflecting the exciting laser beam and a reflection mirror 14 for reflection the exciting laser beam and emitting Stokes light. The resonator 20 for Stokes light comprises a reflection mirror 18 for allowing the transmission of the exciting laser beam and reflecting the Stokes light existing therebetween and the reflection mirror 14 for reflecting the exciting laser beam and emitting the Stokes light. A TEA-CO2 laser 22 is arranged between the reflection mirror 12 and reflection mirror 18 in the resonator 16. The reflection mirror 18 and the reflection mirror 14 are fitted to both end faces of a Raman cell 26 in such a manner that the inside thereof is hermetically sealed. Para-hydrogen is (p-H2 ) is fitted in the Raman cell 26. The optical axis of the exciting laser beam passing the inside of the resonator 16 back and forth and the optical axis of the Stokes light passing the inside of the resonator 20 back and forth are aligned.
    • 7. 发明专利
    • IMAGING METHOD AND DEVICE
    • JPH08279657A
    • 1996-10-22
    • JP10684895
    • 1995-04-06
    • RIKAGAKU KENKYUSHO
    • WADA TOMOYUKITASHIRO HIDEO
    • H01S3/30G01N21/17G01N21/21
    • PURPOSE: To utilize a laser which emits laser pulses whose width is of the order of nanoseconds by a method wherein a coherent image signal component contained in a probe light and a coherent excitation state induced in a Raman medium are made to interact with each other, and only the coherent image signal component is Raman-converted into an anti-Stokes light. CONSTITUTION: Pulse laser beams of a YAG laser 10 are split into two polarized components by a polarizing spectroscope 14, one of the polarized components is made to irradiate a specimen 20 through the intermediary of total reflection mirrors 16 and 18, and the other component is made to impinge on a Raman cell 26 of Raman medium to put the Raman medium in a coherently stimulated state. A probe light which contains the coherent image signal component and the scattered light component of the specimen passing through it is made to impinge on the Raman cell in a coherently stimulated state. The coherent image signal component and the coherently stimulated state are made to interact with each other to Raman-convert only the coherent image signal component into an anti-Stokes light through a filter 28.
    • 9. 发明专利
    • LASER WAVELENGTH CONVERSION AND DEVICE THEREOF
    • JPH0799374A
    • 1995-04-11
    • JP26290593
    • 1993-09-27
    • RIKAGAKU KENKYUSHO
    • TASHIRO HIDEOTSUNEMI AKIRA
    • H01S3/108H01S3/30
    • PURPOSE:To never cause an increase in the size of the whole device and the complification of the whole device, to make it possible to attain a high Raman conversion efficiency and moreover, to reduce a reflection loss in a Raman cell. CONSTITUTION:A laser wavelength conversion device which enters an excitation laser beam into a Raman medium and makes a laser wavelength conversion by performing a Raman conversion, has a resonator, which is constituted of reflecting mirrors 12 and 14 opposing to each other, a laser oscillator 16, which is arranged in the resonator and is filled with a laser medium which generates the excitation laser beam, and a Raman cell 18, which is arranged in the resonator and at the same time, is filled with the Raman medium arranged in such a way as to superpose on one part or all of the optical path of the excitation laser beam which is generated by the oscillator 16. The excitation laser beam generated by the oscillator 16 is made to perform the Raman conversion by the Raman medium in the cell 18 while being made to resonate in the resonator.