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    • 12. 发明专利
    • SUBSTRATE TEMPERATURE MEASURING METHOD
    • JPH1048051A
    • 1998-02-20
    • JP20340896
    • 1996-08-01
    • HITACHI LTD
    • KISHIMOTO SATOSHISHIMAMURA HIDEAKIKOBAYASHI HIDEYONEOKA YUJI
    • G01J5/06G01J5/00
    • PROBLEM TO BE SOLVED: To reduce the number of apparent apertures of a photo-guiding path and to prevent the incident stray light reflected by a wafer surface from reaching a radiation thermometer, by installing a tube having a black inner face, on a part of the photo-guiding path. SOLUTION: A quartz bar 4, a blackbody path 5 and a radiation thermometer 7 are closely installed in series through an opening window 3 of a heat stage 2 on which a wafer 1 is to be placed, so that the stray light does not enter. The length t and the maximum inner diameter ϕ of the blackbody path 5 are set, so that the length t of the blackbody path 5, the maximum inner diameter ϕof the blackbody path 5, the refraction factor n of the quartz bar 4, and the minimum incident angle θ to the photo-guiding path, of the stray light radiation from a heater, reflected by the wafer 1, have the certain relationship. The emissivity of the inner face of the blackbody path 5 is almost 1, so that the infrared ray is emitted from the blackbody itself, and entered into the radiation thermometer 7 as the stray light. For the sake of this, the blackbody path is cooled in a blackbody path cooling part 6, so that the radiation of the inner face of the blackbody path 5 can be made sufficiently smaller than the radiation from the wafer 1.
    • 17. 发明专利
    • DEVICE AND METHOD FOR FORMING WIRING FILM
    • JPH04116828A
    • 1992-04-17
    • JP23562490
    • 1990-09-07
    • HITACHI LTD
    • SHIMAMURA HIDEAKIYAJIMA AKIRAOKAMOTO AKIRAYONEOKA YUJIKOBAYASHI HIDE
    • H01L21/3205H01L21/203H01L21/66H01L23/52H01L23/522H01L23/538
    • PURPOSE:To improve the degree of crystal orientation of a thin film and at the same time, to make it possible to make large the grain diameter of crystal grains by a method wherein a first layer wiring film is formed on a wafer as a seed film in a low-residual gas atmosphere and the first layer wiring film is kept at a temperature higher than the recrystallization temperature of the first layer wiring film. CONSTITUTION:A silicon wafer 4 to be formed with a film is introduced in a load lock chamber 101 at the right end part of a wiring film formation device to evacuate to a vacuum state at a prescribed vacuum degree, then, the wafer 4 is cooled on a cooling stage 200 to a prescribed temperature via a heating chamber 1 and a sputter etching chamber 111 and thereafter, a first layer film which is an Al thin film is formed on the wafer 4 in a first sputter film-forming chamber 201. At this time, the wafer is held at a temperature of 1/2 or lower of the melting point of a first layer wiring film material to form the thin first layer film, this first layer film is heated at a temperature, which is higher than the recrystalline temperature of the first layer film and is lower than the melting point of the first layer wiring film material, and the grain diameter of crystal grains is grown greatly. Then, the crystalline orientation of the thin first layer film is diagnosed with a high-speed electron beam in a treating chamber 202.
    • 19. 发明专利
    • SPUTTERING TARGET
    • JPS62260055A
    • 1987-11-12
    • JP10205186
    • 1986-05-06
    • HITACHI LTD
    • SHIMAMURA HIDEAKIKAWAHITO MICHIYOSHISAKATA MASAOKOBAYASHI HIDEKAMEI TSUNEAKI
    • C23C14/34
    • PURPOSE:To obtain the title target having especially an excellent stepped part covering characteristic and used for a planar magnetron-type sputtering device by providing a groove determined by the radius of gyration of an electron and the thickness of the cathode dark space of electric discharge. CONSTITUTION:The movement of an electron in the space surrounded with >=1 couple of opposed side wall faces 102 formed with protrusions 101 and the sputter face 201 of a target 1 against the directivity of sputtered particles are shown in the figure. Namely, a tunnel-like magnetic field is generated on the face 201, the opposed faces 102 are arranged in the direction to traverse a magnetic flux, and the potentials of the target 1 to be used as a cathode in sputtering and the protrusions 101 are equalized. The space forms a closed loop on the target 1 along the tunnel of the magnetic flux. The electron in the space repeats spiral, drifting, and repulsing movements in relation to the magnetic flux and electric field. When the electron approaches the side wall 102 or target 1, the electron is repulsed as a result of the high negative potentials of the side wall face 102, the target 1 and pushed back to the central part of the space, and hence further stronger plasma is continuously generated.