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    • 111. 发明专利
    • METHOD OF COLLECTING DATA ON BIO-MOLECULE MICRO ARRAY
    • JP2003156442A
    • 2003-05-30
    • JP2001358581
    • 2001-11-22
    • RIKAGAKU KENKYUSHO
    • TASHIRO HIDEOKONDO YASUMITSUKITSUNAI TOKUJI
    • G01N21/64C12N15/09C12Q1/68C40B40/02C40B50/06G01N21/55G01N33/53G01N37/00
    • PROBLEM TO BE SOLVED: To provide a data collection method for DNA micro array capable of collecting automatically fluorescent data from the DNA micro array without troubling a person. SOLUTION: This invention provides the method for collecting data on bio-molecule micro array. A fluorescence-labeled target bio-molecule is interacted with the bio-molecule micro array having a plurality of bio-molecule probe immobilized spots on a light reflecting layer spot on a substrate surface, in the method. The obtained bio-molecule micro array is irradiated with an excitation ray, reflected light and fluorescence from the bio-molecule micro array are measured concurrently, the bio-molecule probe immobilized spots having the light reflecting layer spot is specified based on a difference in intensity of the reflected light on the bio-molecule micro array, and the fluorescent data from a specified spot range is provided. Alternatively, the obtained bio-molecule micro array is irradiated with light, the reflected light from the bio-molecule micro array is measured, the bio-molecule probe immobilized spots having the light reflecting layer spot is specified based on a difference in intensity of the reflected light on the bio-molecule micro array, only a specified bio-molecule probe immobilized spot range is irradiated with an excitation light to measure the fluorescence, and the fluorescent data from the specified spot range are obtained thereby.
    • 116. 发明专利
    • METHOD AND DEVICE FOR PLANE INTERPOLATION OF MEASURED DATA
    • JP2002048524A
    • 2002-02-15
    • JP2000237533
    • 2000-08-04
    • RIKAGAKU KENKYUSHO
    • KASE KIWAMUTASHIRO HIDEO
    • G01B11/24G06T17/00
    • PROBLEM TO BE SOLVED: To allow interpolation processing and rendering based on a large number of three-dimensional data x, y, z under a condition where measured precision of resolution is kept, without changing coordinate values of measured data, to compress the measured data efficiently to reduce a calculation load, and to allow thereby the interpolation processing and the rendering in a short time even in a small-sized computer of a low speed. SOLUTION: This method has a three-dimensional data obtaining step A for obtaining the three-dimensional data of a measured object as two-dimensional coordinates x, y and a height data z, a contour-line processing step B for processing the height data z out of the three-dimensional data by a boundary tracing method to store the data having the same value as a contour line comprising a chain code, a plane interpolation step C for interpolating a space between the contour line in a horizontal face and a vertical face divided into triangles, and a sloped face interpolation step D for substituting a sloped face divided into triangles for an area formed regularly repeatedly with the horizontal faces and the vertical faces at a fixed period.
    • 120. 发明专利
    • LASER OSCILLATION CONTROL METHOD AND ITS DEVICE
    • JP2000022254A
    • 2000-01-21
    • JP18395398
    • 1998-06-30
    • RIKAGAKU KENKYUSHO
    • SATO HIDETOSHIWADA TOMOYUKITASHIRO HIDEO
    • H01S3/117H01S3/136H01S3/137
    • PROBLEM TO BE SOLVED: To prevent emitting laser beams from being affected by a temperature change of an acoustic optical element, by a method wherein an input intensity value of first acoustic waves is set as an input intensity value capable of oscillating a laser, and the input intensity value of second acoustic waves is a value obtained by subtracting the input intensity value of the first acoustic waves from a predetermined value. SOLUTION: A first frequency input from a first RF power source 10 to a piezoelectric element 22 is set as a frequency capable of oscillating a laser in a Ti:Al2O3 laser crystal 14 in response to a frequency of emissive laser beams, and a second RF frequency input from a second power source 12 to the piezoelectric element 22 is set as a frequency incapable of oscillating the laser. And, it is preferable that a first RF input intensity is set to be an intensity most optimal to a laser oscillation of the first RF frequency, but the second RF frequency is controlled so that the total value of the first RF input intensity is always set to be constant. Thus, the emissive laser beams are not affected by a temperature change of a photoacoustic optical element 100.