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    • 61. 发明申请
    • FILM THICKNESS MEASUREMENT DEVICE AND MEASUREMENT METHOD
    • 薄膜厚度测量装置和测量方法
    • US20110299097A1
    • 2011-12-08
    • US13201976
    • 2010-01-20
    • Kenichi OhtsukaTetsuhisa NakanoMotoyuki Watanabe
    • Kenichi OhtsukaTetsuhisa NakanoMotoyuki Watanabe
    • G01B11/28
    • G01B11/0633G01B11/0683
    • A film thickness measurement apparatus 1A includes a measurement light source 28 that supplies measurement light containing a measurement light component with a first wavelength λ1 and a measurement light component with a second wavelength λ2 to a measuring object 15, a spectroscopic optical system 30 that decomposes interfering light of reflected light from the upper surface and reflected light from the lower surface of the measuring object 15 into an interfering light component with the first wavelength λ1 and an interfering light component with the second wavelength λ2, photodetectors 31 and 32 that detect intensities of the first and second interfering light components at each time point, and a film thickness analysis section 40. The film thickness analysis section 40 obtains a temporal change in film thickness of the measuring object 15 based on a phase difference between a first phase in a temporal change in detected intensity of the first interfering light component and a second phase in a temporal change in detected intensity of the second interfering light component. Accordingly, a film thickness measurement apparatus and a film thickness measurement method by which a temporal change in film thickness of a film-shaped measuring object can be accurately measured are realized.
    • 膜厚测量装置1A包括测量光源28,该测量光源28将包含第一波长λ1的测量光分量和具有第二波长λ2的测量光分量的测量光提供给测量对象15;分光光学系统30,其分解干涉 来自上表面的反射光和来自测量对象15的下表面的反射光成为具有第一波长λ1的干涉光分量和具有第二波长λ2的干涉光分量,光电探测器31和32检测强度 每个时间点的第一和第二干涉光分量以及膜厚度分析部分40.薄膜厚度分析部分40基于时间变化中的第一相位之间的相位差来获得测量对象15的膜厚度的时间变化 在第一干涉光分量的检测强度 在第二干涉光分量的检测强度的时间变化中相位相位。 因此,可以实现膜厚测量装置和薄膜厚度测量方法,通过该方法能够精确地测量薄膜状测量对象的膜厚度的时间变化。
    • 66. 发明授权
    • Semiconductor laser device
    • 半导体激光器件
    • US5020072A
    • 1991-05-28
    • US401745
    • 1989-09-01
    • Yuji AbeHiroshi SugimotoKenichi OhtsukaToshiyuki OishiTeruhito Matsui
    • Yuji AbeHiroshi SugimotoKenichi OhtsukaToshiyuki OishiTeruhito Matsui
    • H01S5/00H01S5/12
    • H01S5/12H01S5/1231H01S5/124H01S5/1243
    • A semiconductor laser device includes an active layer, a first semiconductor layer having a larger energy band gap than the active layer, a diffraction grating layer having a larger energy band gap than the active layer and a smaller energy band gap than the first semiconductor layer, and a second semiconductor layer having the same composition as the first semiconductor layer, successively grown on the active layer, parallel stripe grooves of predetermined period reaching the first semiconductor layer produced at the entire surface of the grown layers, a cladding layer having the same composition as the first semiconductor layer which is re-grown thereon, and a diffraction grating constituted by the remainder of the diffraction grating layer. The coupling coefficient of the light is determined by the film thickness of a layer produced between the active layer and the diffraction grating layer, and the amplitude of the diffraction grating is determined by the layer thickness of the diffraction grating layer. Therefore, the coupling coefficient can be set at a design value at high precision and at high reproducibility.
    • 半导体激光器件包括有源层,具有比有源层大的能带隙的第一半导体层,具有比有源层更大的能带隙的衍射光栅层和比第一半导体层更小的能带隙, 以及具有与第一半导体层相同的组成的第二半导体层,在有源层上依次生长,在生长层的整个表面上到达第一半导体层的预定周期的平行条纹沟槽,具有相同组成的包覆层 作为在其上重新生长的第一半导体层,以及由衍射光栅层的其余部分构成的衍射光栅。 光的耦合系数由有源层和衍射光栅层之间产生的层的膜厚决定,衍射光栅的振幅由衍射光栅层的层厚决定。 因此,可以以高精度和高重现性将耦合系数设定在设计值。