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    • 63. 发明专利
    • HEATING UNIT WITH BUILT-IN OPTICAL FIBER
    • JPH06267642A
    • 1994-09-22
    • JP5356293
    • 1993-03-15
    • HITACHI LTDHITACHI NUCLEAR ENG
    • ONISHI TAKESHIKAWAMOTO KIKUOABE SHIGEKI
    • F16L53/00G01K11/12H05B3/56
    • PURPOSE:To reduce a temperature measuring unit, to simplify the system, and to improve the control property, by detecting the heating temperature heated by a resistance element provided in parallel between two power source wires, by an optical fiber provided parallel to the power source wires. CONSTITUTION:To a belt form heating unit 1, AC power sources R and S are applied through two power source wires 3. This voltage is transmitted through the power source wires 3, and transmitted to resistance elements 4 provided in parallel to the wires 3 in the longitudinal direction, and a current according to the resistant value flows to heat the resistances 4. This temperature is detected by an optical fiber 2 provided parallel to the power source wires 3. The heating elements 3 and 4, and the optical fiber 2 are housed in a sheath member 5 and integrated. The optical fiber 2 can measure the peripheral temperature at 1m pitch, and by laying the the optical fiber 2 in the same route of the heating elements, the distribution of the temperature around the heating unit 1 in the longitudinal direction can be measured. Consequently, the temperature measuring unit can be reduced, and the control property can be improved.
    • 65. 发明专利
    • SAMPLE PROCESSOR USING CHARGED BEAM
    • JPH06215723A
    • 1994-08-05
    • JP733393
    • 1993-01-20
    • HITACHI LTD
    • SATO HITOMIISHITANI TORUONISHI TAKESHI
    • H01J37/22H01J37/30
    • PURPOSE:To facilitate the designation of a point of beam radiation at the time of processing either by displaying very small difference in the intensity of secondary electrons in terms of drastically different color or by displaying the intensity of the secondary electrons in terms of concentration of the color to display only a specific range of intensity by a color totally different from the entire gradation. CONSTITUTION:When a display color corresponding to the intensity of secondary electrons is designated by using a color lookup table CLT, a part where the variation in the intensity is very small, for example, when it varies from (i) to (j), the display colors of the CLT are designated so that distinct color variation such as red, blue, green, is displayed, namely, a:b:cnot equal to a':b':c'. After deep color gradation is designated when the intensity value of secondary electrons is large, or light color gradation when the value is small, the display colors that are only in a specific intensity range in which the intensity varies from (i) to (j), are replaced with a color B which is totally different from the entire color gradation. Even in a part where the variation in the intensity of secondary electrons is very small, or in a part where the part indicating variation is very small, they can be recognized on a CRT, and a point of radiation can thus be easily designated at the time of ion beam processing.
    • 70. 发明专利
    • CONVERGED ION BEAM PROCESSING DEVICE
    • JPH04262354A
    • 1992-09-17
    • JP2310191
    • 1991-02-18
    • HITACHI LTD
    • ONISHI TAKESHIISHITANI TORU
    • H01J37/22H01J37/28H01J37/30
    • PURPOSE:To make accurate location of the processing position even in case a device involves parts with extremely different secondary electron discharging rate within the observing field of view by providing a means to compress the secondary particle intensity logarithmically for imaging. CONSTITUTION:An ion beam emitted by a liquid metal ion source 100 is converged on a specimen 8 by a condenser lens 101 and an objective lens 107. Secondary electrons generated by the specimen 8 when it is irradiated with this converged ion beam (FIB) are sensed and amplified by a secondary electron sensor 7 and are synchronized with the deflection control to be displayed as a scan ion microscope image (SIM) on CRT 5 of a computer 4. A current signal emitted by the sensor 7 is connected either with a linear amplifier 2 or a logarithmic amplifier 1 through a changeover switch 6. Accordingly a SIM image as logarithmic indication of the secondary electron signal amount is obtained by turning the switch 6, which permits observing the shape of the device over the whole area of the screen. Thus the location of the processing position can be made accurately.