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    • 2. 发明专利
    • MASS SPECTROMETER
    • JP2000223065A
    • 2000-08-11
    • JP1944699
    • 1999-01-28
    • HITACHI LTD
    • YAMAGUCHI HIROKATSUEGUCHI KINYASAKIMOTO MASANORI
    • H01J49/06G01N27/62H01J49/40
    • PROBLEM TO BE SOLVED: To provide a small device for analyzing a surface by loading a large sample on a sample stage as it is, by providing a rear-stage reflection electrode on an ion track in order to guide ions ejected from an ion reflector to a detector. SOLUTION: Laser beams going out of a laser beam source 3 are reflected by a mirror 6 having a through hole, and are focused onto a sample 2 by an objective lens 5. Ions generated with irradiation are accelerated by an ion drawing electrode 8, and are guided to this flight-time-type mass spectrometer 1. A polarization electrode 11 is adjusted so as to direct a progressing direction of the ions to an ion reflector (reflectron) 9. The ions reflected by the reflectron 9 are reflected by a rear-stage reflection electrode 40, and focused by an ion lens 41, and are detected by an ion detector 10. Masses are determined by measuring a time required from laser oscillation to arrival at the ion detector 10. By reflecting the ions with the rear-stage reflection electrode 40, the detector 10 can be placed at a position away from a sample container 20, and measurement of a large sample is allowed.
    • 4. 发明专利
    • MASS SPECTROMETER
    • JPH0945276A
    • 1997-02-14
    • JP19143295
    • 1995-07-27
    • HITACHI LTD
    • AKAMATSU NAOTOSHIEGUCHI KINYAYAMAGUCHI HIROKATSU
    • G01N27/62H01J49/10H01J49/40
    • PROBLEM TO BE SOLVED: To reduce a focusing diameter through the application of a laser beam from the vertical direction and to enhance image resolution by opposing a microscope to a sample, and causing ions to fly crosswise by means of ion accelerating electrodes. SOLUTION: A sample 2 is inserted between accelerating electrodes 22. During mass spectrometry, a laser beam 7a from a laser beam source 6 is focused onto the sample 2 by a condensing lens 22. An ion beam 21b excited thereby is accelerated by an accelerating electrode 40 in an almost perpendicular direction to the direction of incidence of the laser beam and is made to impinge on a mass spectrometer part 1. The ion beam 21b is reflected by an ion reflector 30 and impinges on an ion detecting part 34. Ion flight time can be obtained by measuring the time from the application of the laser beam 7b to the arrival of the ions at the ion detector 34. Mass spectrometry of the ions can thus be performed. During observation of the sample, light from a sample illuminating light source 8 is made to impinge on the sample 2 from the condensing lens 22. An image of the sample 2 formed thereby is observed with a TV camera 10.
    • 5. 发明专利
    • SAMPLE ANALYZING DEVICE AND METHOD
    • JPH08193979A
    • 1996-07-30
    • JP691595
    • 1995-01-20
    • HITACHI LTD
    • OSHIDA YOSHITADAEGUCHI KINYAMIZUNO FUMIONOZOE MARISUGIMOTO ARITOSHI
    • G01N27/62G01N1/00G01N21/71H01L21/66
    • PURPOSE: To analyze a fine pattern defect and the constituent of a fine adhered foreign object by opening a hole at a tip lens facing the sample of a transmission-type optical system and passing a vaporized atom, molecule, or ion and leading it to an analyzing system. CONSTITUTION: Holes 231 and 232 with a lens light axis nearly as the center are opened at tip lenses 201 and 202 facing a sample 1 of a transmission-type optical system 2 with a large pupil diameter. When light is applied from a laser light source 3, beams are of donut shape by a pupil-conjugate filter 34, form an image on the pupil of an optical system 2 by lenses 35 and 21, do not hit against the side surface of the holes 231 and 232, cause a small spot close to a diffraction limitation determined by the numerical aperture of the optical system 2 to be formed on the surface of the sample 1, and allow an object on the surface of the ionized sample 1 to be guided to a flight-time-type mass analyzer 8 through the holes 231 and 232. As a result, the transmission-type optical system 2 with a large numerical aperture can be arranged nearly vertically to the sample 1, thus applying light with a smaller spot size and selectively vaporizing a fine region.
    • 9. 发明专利
    • INFRARED ABSORPTION SPECTRUM REFLECTING AND MEASURING APPARATUS
    • JPS6375642A
    • 1988-04-06
    • JP21959886
    • 1986-09-19
    • HITACHI LTD
    • EGUCHI KINYANIITSUMA KIKUEWAKANA SHIGERUEZAWA MASAYOSHI
    • G01N21/3563G01N21/35G01N21/47
    • PURPOSE:To measure an infrared spectrum with high sensitivity by guiding infrared rays to the minute part of a specimen while reducing the scattering thereof, by guiding infrared rays to a fine pipe made of gold or having a gold plated inner surface to irradiate the specimen and condensing the reflected light from the specimen to a detector through an eccentric type ellipsoidal reflecting mirror. CONSTITUTION:The tille apparatus measures an infrared absorption spectrum according to a reflecting method and is especially adapted to a minute point infrared reflecting spectral apparatus requiring high brightness infrared rays. That is, the infrared rays 2 from an infrared rays source pass through a pipe (light pipe) made of gold without generating scattering to irradiate the extremely minute point of a specimen 3 to be analyzed. The incident angle of said infrared rays at this time is set to 45 deg.. The measuring part of the specimen 3 to be analyzed is present at the almost one focus position of an eccentric type ellipsoidal reflecting mirror 4 constituting a reflected light condensing system and the reflected light from the specimen 3 to be analyzed is condensed to a detector 5 by the eccentric type ellipsoidal reflecting mirror 4.
    • 10. 发明专利
    • METHOD FOR MEASURING TOTAL REFLECTION INFRARED ABSORPTION SPECTRUM
    • JPS61281946A
    • 1986-12-12
    • JP12245085
    • 1985-06-07
    • HITACHI LTD
    • ISHIKAWA MEGUMIEGUCHI KINYA
    • G01N21/27G01N21/35G01N21/552
    • PURPOSE:To analyze the depth in a total IR light wavelength region at one time by using an inorg. compd. having no absorption in the wavelength region of IR light as a spacer. CONSTITUTION:The IR light 2 emitted from an IR light source 1 passes through a Michelson interferometer 3, is made incident on a crystal 5 in a sample holder 4 and is totally reflected by the boundary between the crystal 5 and the spacer 6. The inorg. compd. such as ZnSe or PbF2 which has the refractive index lower than the refractive index of the crystal 5 and is transparent to IR light is used for the spacer 6. Part 7 of the incident IR light bleeds to a measuring sample 8 beyond the boundary, is reflected by receiving the effect of the absorption by the sample 8 and is detected by a detector 9. The detected light is processed by a data processor 10 and the total reflection IR absorption spectrum is obtd. The penetration depth of the IR light 7 penetrating into the sample 8 in the stage of total reflection changes when the thickness of the spacer 6 is changed. The depth analysis is thus made possible. The depth in the total IR wavelength region is thereby analyzed without receiving the effect of absorption by the spacer.