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    • 85. 发明专利
    • DIFFUSED REPLENISHING ELECTRON SOURCE AND MANUFACTURE THEREOF
    • JPH0935674A
    • 1997-02-07
    • JP17980295
    • 1995-07-17
    • HITACHI LTD
    • SHINADA HIROYUKIFUKUHARA SATORUKURODA KATSUHIRO
    • H01J37/06H01J1/15H01J1/304H01J1/30
    • PROBLEM TO BE SOLVED: To provide a diffused replenishing electron source with high brightness and a long life by connecting a high melting point metal single crystal wire to the tip of a high melting point metal filament, and applying slurry prepared with replenishing source powder and a nitrocellulose-containing organic solvent to the connecting part. SOLUTION: A single crystal wire made of a high melting point metal having an axial orientation of is connected to the peak of the central end binding part of a filament 2 made of high melting point metal, then a single crystal chip 1 is formed by electrolytic polishing. Slurry prepared with replenishing source powder 3 and a nitrocellulose-containing organic solvent (isoamyl acetate or the like) is applied to the connecting part of the filament 2 and the single crystal chip 1, then they are heated in vacuum to sinter the replenishing source powder 3. The filament 2 and the single crystal wire are made of a fine wire of either one of W, Mo, and Re, and the replenishing source powder is made of the powder of at least one metal selected from the group comprising Ti, Zr, Hf, Y, Th, Sc, Be, and Ba. A diffusion replenishing type electron source with high stability and high production yield can be obtained.
    • 87. 发明专利
    • CHARGED PARTICLE DEVICE
    • JPH0864161A
    • 1996-03-08
    • JP20042494
    • 1994-08-25
    • HITACHI LTD
    • KAMIYAMA REIKOESUMI MAKOTOFUKUHARA SATORUTODOKORO HIDEO
    • H01J37/04
    • PURPOSE: To shorten the time required for control by previously measuring the variation range of electron beam amounts corresponding to the variation range of control voltage in which an optical axis is not varied and controlling the electron beam amount based on the measured value. CONSTITUTION: An electron beam drown with a drawing voltage 4 is adjusted with control voltage 3, then accelerated with accelerating voltage 6. The electron beam amount is measured with a Faraday cup 7. The electron beam amount is reversely proportional to the control voltage 3, and the range of the electron beam amount is decided with the range of the control voltage. As this method, the electron beam amount serving as the reference is set, and the drawing voltage 4 until the electron beam amount reaches the set value is adjusted for axial adjustment. The control voltage 3 is increased to the maximum value already set, and the electron beam amount at this point of time is measured with the Faraday cup 7. The voltage 3 is decreased to the minimum value already set, and the electron beam amount is measured. This electron beam amount is stored as the maximum value, and the maximum value and the minimum value are displayed as the range of the electron beam amounts.
    • 90. 发明专利
    • ROTARY CENTER DETECTING METHOD FOR CHARGED PARTICLE BEAM DEVICE
    • JPH0349144A
    • 1991-03-01
    • JP18270189
    • 1989-07-17
    • HITACHI LTD
    • SHINADA HIROYUKITODOKORO HIDEOFUKUHARA SATORUOTOMO MOICHIKIYOFUJI SHIGEMITSU
    • H01J37/147G11B5/455H01J37/28
    • PURPOSE:To precisely determine the positional relation between the rotary center of a sample and an electron beam by calculating the rotary center of the sample based on the deflection quantity data at the rotating angle 0 deg. and the deflection quantity data at 180 deg.. CONSTITUTION:When an electron beam 2 is scanned in the X-direction in a scanning range 22 and its position is measured by the position detector 7 of the charged particle beam 2, a signal wave form reflected with the distribution of the magnetic field strength of a magnetic head 5 is obtained. When the head 5 is rotated 180 deg. around a rotary center 21 perpendicular to the incident direction of the beam 2 and the position is likewise measured, a wave-form reversed with the previously measured wave- form is obtained because only the incident direction of the beam 2 is reversed and the passing path of the beam 2 is the same as that at the rotating angle 0 deg.. When both wave-forms are displayed while the scanning position in the X-direction of the beam 2 is shown on the horizontal axis and the position change in the Y direction of the beam 2 is shown on the vertical axis, two wave-forms are made point- symmetrical, and the center coincides with the X-coordinate of the rotary center of a sample. The positional relation between the scanning range 22 of the beam 2 and the rotary center 21 of the sample is clarified.