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    • 1. 发明专利
    • SEPARATING AND RECOVERING DEVICE FOR METAL
    • JPS6415333A
    • 1989-01-19
    • JP16914387
    • 1987-07-07
    • JAPAN ATOMIC ENERGY RES INSTISHIKAWAJIMA HARIMA HEAVY IND
    • SHIBA YOSHIYUKIARISAWA TAKASHISHIBATA TAKEYORIDOI TAKESHIKADOI HIDEO
    • C22B9/02
    • PURPOSE:To recover separated, evaporated metal by liquid carrier metal and continuously take it out by letting liquid carrier metal flow uniformly from the high level side to the low level side on the liquid carrier metal holding part under an inclined evaporated metal recovering plate. CONSTITUTION:A metal 29 to be evaporated in an evaporation crucible 2 is heated and evaporated by irradiating electron rays from an electron gun 3 in a vacuum container 1. After passing a focusing device 4, a laser beam 5 of a specific frequency is projected on this evaporated metal and metal to be separated is ionized selectively. Then, electrolytic metal is adsorbed by a recovering plate 7, separated and recovered. Neutral evaporating metal is brought into contact with the lower surface of a neutral metal recovering plate 8 which is inclined by a prescribed angle. The lower surface of this recovering plate 8 is covered with stretched wire, etc., as a liquid carrier metal holding structure and liquid carrier metal is poured uniformly from the high level side to the low level side in a storing tank 16. Said neutral evaporated metal is recovered by this carrier metal, flows and is taken out outside the vacuum container 1 through a recovering through 19, a recovering tank 20, a duct 21 and separated recovered by a neutral metal separating and refining device 22 from the carrier metal.
    • 4. 发明专利
    • ISOTOPE SEPARATION DEVICE
    • JPH01293124A
    • 1989-11-27
    • JP12353488
    • 1988-05-20
    • JAPAN ATOMIC ENERGY RES INST
    • SHIBATA TAKEYORIMUKODA HIDETOSHI
    • G21G1/00B01D59/34
    • PURPOSE:To allow to project an electron beam to the surface of metallic material without undergoing irregular disturbance by forming the magnetic shield which shields the electron beam from the deflecting magnetic field with a high temp. superconductive body. CONSTITUTION:A magnetic shield 11 shielding the magnetic field in the vicinity of beam orbit is provided at the beam projecting opening of an electron gun 3 in order to introduce the electron beam 4 in a straight line as far as the vicinity of a crucible 2. The magnetic shield 11 is formed of a high temp. superconductive body. Consequently, the magnetic field surrounding the magnetic shield 11 can not put the inside of the magnetic shield 11 into effect due to the Meissner effect of high temp. superconductive body with the result that the inside of the shield has uniform magnetic field distribution. As a result, the electron beam 4 left from the magnetic shield is preferably introduced to the surface of a metallic raw material 1 by the deflecting magnetic field.
    • 5. 发明专利
    • GAS CHROMATOGRAPH
    • JPS62278452A
    • 1987-12-03
    • JP12189986
    • 1986-05-27
    • JAPAN ATOMIC ENERGY RES INST
    • SHIBATA TAKEYORITANASE MASAKAZU
    • G01N30/54B01D15/08B01D59/26
    • PURPOSE:To achieve a higher resolution, by employing a closed type liquefied gas container for immersing a column to vary the temperature thereof with the control of the pressure of a liquefied gas. CONSTITUTION:A container 5 for a liquefied gas 4 such as liquefied nitrogen shall be of a closed type with a lid 7 and a pressure of an evaporated gas 8 in the liquefied gas 4 is detected with a manometer to adjust the opening of a release value 10 so that the pressure will allows a set temperature of a column 2 to reach the boiling point of the liquefied gas 4. A thermometer 11 such as thermocouple is provided at a lower part of the liquefied gas 4 to keep the temperature of the liquefied gas 4 from falling below the boiling point thereof and a heater 12 placed at a lower part of the liquefied gas 4 is electrically energized to raise the temperature up to the boiling point with the evaporation of the liquefied gas 4. To lower the pressure of the liquefied gas 4 and the evaporated gas 8 below the atm., the evaporated gas 8 from the release valve 10 is discharged with a vacuum discharge pump.
    • 10. 发明专利
    • MEASURING METHOD FOR VAPOR DENSITY DISTRIBUTION
    • JPS62255848A
    • 1987-11-07
    • JP9852186
    • 1986-04-28
    • JAPAN ATOMIC ENERGY RES INST
    • SHIBATA TAKEYORISUZUKI YOUJI
    • G01N21/62G01N9/00
    • PURPOSE:To easily measure a distribution of a vapor density by exciting the vapor in a vacuum container with a light beam, an electron beam, an ion beam, etc., to cause it to emit a light beam, and observing the emitted light at each plate by a TV camera. CONSTITUTION:The whole light emitting part is made to form an image on a two-dimensional multi-channel photodetector 11 of a TV camera 9 by a lens 10 of the TV camera 9 through a large window 8. The quantity of light which enters into each channel is proportional to a density of each part of the light emitting part. Also, the quantity of light which enters into each channel is a video signal of the TV camera 9, and by fetching directly this signal from a TV camera controller 12, a vapor density can be derived. Moreover, by storing the video signal in a digital video memory 14 and processing it by a computer 15, a vapor density distribution can be obtained. Also, when a filter 16 for making only a light beam emitted from vapor pass through is placed on the way from an optical path, stray light can be prevented, and the vapor density distribution can be derived more exactly.