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    • 3. 发明专利
    • Electronic equipment utilizing uwb communication
    • 电子设备利用UWB通信
    • JP2005086685A
    • 2005-03-31
    • JP2003318742
    • 2003-09-10
    • Mitsubishi Electric Corp三菱電機株式会社
    • MURAKAMI TAKAAKIFURUKAWA AKIHIKOTOMIZAWA ATSUSHIOMORI TATSUO
    • H04B1/38
    • PROBLEM TO BE SOLVED: To enable devices arranged inside a case to communicate one another by UWB technique without being affected by structure inside the case in electronic equipment, such as a personal computer.
      SOLUTION: The electronic equipment comprises: a first UWB communication chip set 31 including a first antenna 312; a second UWB communication chip set 32 including a second antenna 322; and the case 6 for UWB communication that is a case for allowing the inside space to be continuously, electromagnetically isolated from the periphery. The first and second antennas 312, 322 are arranged so that they perform UWB communication each other via the inside space of the case 6 for UWB communication.
      COPYRIGHT: (C)2005,JPO&NCIPI
    • 要解决的问题:使得布置在壳体内的装置能够通过UWB技术彼此通信而不受诸如个人计算机之类的电子设备中的壳体内的结构的影响。 电子设备包括:包括第一天线31​​2的第一UWB通信芯片组31; 包括第二天线322的第二UWB通信芯片组32; 以及用于允许内部空间连续地与外围电磁隔离的情况的用于UWB通信的情况6。 第一和第二天线312,322被布置成使得它们经由用于UWB通信的壳体6的内部空间来执行UWB通信。 版权所有(C)2005,JPO&NCIPI
    • 5. 发明专利
    • ION SOURCE
    • JPH02301940A
    • 1990-12-14
    • JP12305989
    • 1989-05-17
    • MITSUBISHI ELECTRIC CORP
    • ONO KOICHIOMORI TATSUO
    • H01J27/08H01J27/20H01J37/08
    • PURPOSE:To make it possible to apply the generation of low energy ion beams and convergent ion beams to ultra high brightness ion beams by extracting ion current from the super-sonic molecule flow of plasma obtained from super- sonic expansion taking a place when plasma generated in a discharge chamber is introduced into a vacuum chamber. CONSTITUTION:Plasma composed of specimen gas B generated in a discharge chamber 1 and of carrier gas A, flows out into the first vacuum chamber 22 through a nozzle 26 so as to be super-sonically expanded so that the super-sonic free jet steam D of plasma is thereby formed. In the second place, a section close to the center axis of the super-sonic free jet stream D of plasma in a region of stillness is extracted out as super-sonic molecule flow E into the second vacuum chamber 23 by means of a skimmer 28 provided for the first bulkhead 27. The super-sonic molecule flow E passes through a collimator 30 provided for the second bulkhead 29 so as to flow in the third vacuum chamber 24. Plasma ions are extracted as ion current F out of an electric hole 8 while being accelerated to the direction of an electrode 7 by means of the electric field applied between the collimator 30 and the electrode 7.
    • 6. 发明专利
    • MANUFACTURE OF OXIDE SUPERCONDUCTIVE THIN FILM
    • JPS6460926A
    • 1989-03-08
    • JP21889087
    • 1987-08-31
    • MITSUBISHI ELECTRIC CORP
    • ONO KOICHIOMORI TATSUOFUJITA SHIGETO
    • H01B12/06C30B29/22H01B13/00H01L39/24
    • PURPOSE:To enhance the thin film growing speed by introducing a test gas containing powder of oxide superconductive component material in plasma, and by spraying the plasma having gasified oxide superconductive component material to the base board. CONSTITUTION:Vacuum exhaust is made from a vacuum draw hole 7, and a gas 8, for ex. argon gas, is introduced to a discharge chamber 1 from a main gas lead-in hole 6, and a DC voltage is impressed between a cathode 2 and an intermediate electrode 10. This gas is electrolytically dissociated by glow discharge or arc discharge generated between the cathode 2 and intermediate electrode 10 and turned into plasma. It passes through an intermediate electrode hole 11 and flows into the space between the intermediate electrode 10 and anode 4. Test gases 16-18 containing component material powder for oxide superconductor, for ex. lanthanum oxide, and argon gas to carry it are led in from test gas lead-in holes 13-15. The gases become plasma, and the powder is gasified. This mixed plasma flows into a vacuum chamber 12, and electrolytic dissociated gas jet 19 is formed. An oxide superconductive thin film is grown on a base board arranged oppositely.
    • 8. 发明专利
    • DETECTOR FOR END POINT PLASMA ASHING
    • JPS62250644A
    • 1987-10-31
    • JP9432186
    • 1986-04-23
    • MITSUBISHI ELECTRIC CORP
    • OMORI TATSUOONO KOICHIFUJITA SHIGETO
    • H01L21/302H01L21/3065
    • PURPOSE:To detect the end point of ashing precisely and stably by detecting the intensity of light of at least two or more of spectral lines in transition light within a specific wave range from 0H (hydroxyl group molecule) in plasma and comparing the intensity of these light. CONSTITUTION:In a plasma ashing end-point detector, the angle of rotation of a diffraotion grating 15 is changed and some spectral line in SIGMA - pi transition light within the range of wavelengths 306-316nm from OH is extracted, the spectral line is projected to a photo multiplier 17, the intensity of light of the spectral line is converted into electric signals, and the maximum value Ia of the electric signals is memorized temporarily in a detector 13. The diffraction grating 15 is turned, another spectral line is selected similarly, and the maximum value Ib of the spectral line is memoriz ed into the detector 13. The rotational temprature of plasma is obtained from the ratio of the intensity of these two maximum values, and the variation of a rotational temperature in the vicinity of an organic film and the rotational temperature of a plasma region in the vicinity of an electrode is compared from the alteration of the rotational temperature of plasma or by mounting two monochromators 14, thus detecting the end point of ashing.
    • 9. 发明专利
    • DETECTOR FOR END POINT OF PLASMA ASHING
    • JPS62250640A
    • 1987-10-31
    • JP9432086
    • 1986-04-23
    • MITSUBISHI ELECTRIC CORP
    • OMORI TATSUOONO KOICHIFUJITA SHIGETO
    • H01L21/302H01L21/3065
    • PURPOSE:To detect the end point of ashing precisely and stably by detecting the intensity of light of at least two or more of spectral lines in transition light within a specific wave range from C0 in plasma and comparing the intensity of these lights. CONSTITUTION:The angle of rotation of a diffraction grating is changed and some spectral line in b SIGMA-a pi transition light within the range of wavelengths 296-300nm from CO is extracted, and the spectral line is projected to a photomultiplier 17, the intensity of light is converted into electric signals, and the maximum value of the electric signals is memorized temporarily in a detector 13. The diffraction grating 15 is turned, another spectral line is selected similarly, and the maximum value of the spectral line is memorized to the detector 13. The rotational temperature of plasma is obtained from the ratio of the intensity of these two maximum values, and the variation of a rotational temperature in the vicinity of an organic film and the rotational temperature of a plasma region in the vicinity of an electrode is compared from the alteration of the rotational temperature of plasma or by mounting two monochromators 14, thus detecting the end point of ashing. Accordingly, the adjustment of the detector by the change of the conditions of ashing is unnecessitated, thus stably detecting the end point of ashing accurately.
    • 10. 发明专利
    • ION SOURCE
    • JPS6217935A
    • 1987-01-26
    • JP15657085
    • 1985-07-15
    • MITSUBISHI ELECTRIC CORP
    • ONO KOICHIOMORI TATSUOFUJITA SHIGETO
    • H01J27/02H01J37/08
    • PURPOSE:To obtain a gas ion source applicable onto super high brightness ion beam by leading the weakly ionized gas produced from weakly ionized gas producing means through a hole of barrier board into first vacuum chamber than expanding freely with supersonic speed while arranging plural take-out electrodes having a hole at low gas temperature area of said freely expanded flow and taking ion flow into second vacuum chamber. CONSTITUTION:Ion source is provided with discharge chamber 1 and vacuum chambers 2, 3. The vacuum chamber 2 is maintained at higher vacuum than the discharge chamber 1 while the vacuum chamber 3 is maintained at higher vacuum than the vacuum chamber 2. The discharge chamber 1 is provided with a cathode 4, an intermediate electrode 5 and an anode 6. The intermediate electrode 5 is provided with an intermediate electrode hole 7 while the anode 6 is provided with an anode hole 9. The vacuum chamber 2 will contact through the anode 6 with the discharge chamber 1 while communicate through the anode hole 9 with the discharge chamber 1. Take-out electrodes 14a, 14b for taking out ion flow from weakly ionized freely expanded gas flow formed in the vacuum chamber 2 are arranged between the vacuum chambers 2, 3. The take- out electrodes 14a, 14b are provided with take-out electrode holes 15a, 15b for passing ions.