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    • 3. 发明专利
    • COLOR CHANGEABLE GLOVE
    • JPH04127098A
    • 1992-04-28
    • JP24816490
    • 1990-09-18
    • POWER REACTOR & NUCLEAR FUEL
    • TAKAHASHI YOSHIHARU
    • G21F7/04B25J21/02
    • PURPOSE:To quickly make possible the discovery of a damage part by visual observation if the damage part should occur in a glove by providing a transparent (or semitranspaent) layer positioned on the surface and a changeable color layer changed by the change of pH in contact therewith. CONSTITUTION:A first layer 11 positioned on the surface consists of a transparent or semitranparent buck-up material, a second layer 12 is composed of a changeable material containing a color changing raw material by the use of the change of pH and a third layer 13 consists of a constitutive material of a glove body. By this constitution, when a layer composed of the constitutive material of the glove body is exposed under outside environment to produce a pin hole and quality inferiority in use, chemicals are invaded from the damage part 14. Thereby, since the raw material of pH indication in a color changeable layer is color-changed, the damage part 14 can be discovered easily.
    • 6. 发明专利
    • HIGH-REPETITION RAMAN LASER DEVICE
    • JPH0456184A
    • 1992-02-24
    • JP16361490
    • 1990-06-21
    • POWER REACTOR & NUCLEAR FUEL
    • MIYAMOTO YASUAKISUDO OSAMUHASEGAWA MAKOTO
    • G02F1/35B01D59/00B01D59/34B01D59/44H01S3/30
    • PURPOSE:To enable non-uniform fluctuation which is generated in Raman conversion medium to be eliminated, its relaxation to be promoted, high-repetition oscillation to be stabilized, and energy to be saved by providing a multi-bus cell for non-saturation conversion and a multi-bus cell for saturation conversion. CONSTITUTION:A Raman conversion multi-bus cell consists of two parts 1 and 3, where one multi-bus cell is a multi-bus cell for non-saturation conversion 1 and temperature conditions etc., can be set freely. On the other hand, the other multi-bus cell is the multi-bus cell for saturation conversion 3 and flow of para-hydrogen is produced within this cell 3 only. Then, Raman conversion of paths excluding 2-3 paths before Stokes light power is saturated and immediately before saturation is performed within the cell 1 and then 2-3 paths immediately before saturation are performed within the cell 3 through a collimator 5 or a mirror system 5, thus enabling fluctuation which is generated due to cooling accompanying Raman conversion to be eliminated or the relaxation to be promoted, a stable and high-repetition Stokes light oscillation to be achieved, and a highly efficient conversion to be made.
    • 9. 发明专利
    • MULTIMODE RAMAN LASER SYSTEM
    • JPH03280485A
    • 1991-12-11
    • JP8190690
    • 1990-03-28
    • RIKAGAKU KENKYUSHOPOWER REACTOR & NUCLEAR FUEL
    • TASHIRO HIDEOMIDORIKAWA KATSUMISUZUKI YOSHIHISA
    • B01D59/34H01S3/30
    • PURPOSE:To improve a multimode Raman laser system in conversion efficiency and to dispense with an amplifier constituted in multistage by a method wherein an unstable resonator type oscillator is used as a TEA CO2 laser device, and a multimode Raman cell is employed as a Raman cell. CONSTITUTION:An unstable resonator type oscillator is used as a TEA CO2 laser device 11, and a single longitudinal mode CW-CO2 laser device 2 is employed as an injection light source of feeble circular polarized light. A circular polarized high power laser beam emitted from the TEA CO2 laser device 11 is injected into a multimode Raman cell 16. The multimode Raman cell 16 is composed of an SUS pipe with a pair of concave mirrors provided to both its ends respectively, where a laser beam injection hole 17 and a laser beam output hole 18 are provided to the concave mirrors respectively and the SUS pipe is charged with parahydrogen gas. A circular polarized high power laser beam incident through the laser beam injection hole 17 induces scattered light 16mum in wavelength through a Raman effect of parahydrogen as being repeatedly reflected by a pair of concave mirrors, and the scattered light is emitted through the laser beam output hole 18.