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    • 91. 发明授权
    • Optical device with improved focused error detection and tracing error
detection for optical disk drive
    • 具有改进的光盘驱动器的聚焦误差检测和跟踪误差检测的光学装置
    • US5754503A
    • 1998-05-19
    • US749231
    • 1996-11-14
    • Satoshi SenbaShinya HasegawaHiroyasu YoshikawaFumihiro Tawa
    • Satoshi SenbaShinya HasegawaHiroyasu YoshikawaFumihiro Tawa
    • G11B7/09G11B7/135G11B7/00
    • G11B7/1353G11B7/0908G11B7/0916
    • An optical device for an optical disk drive, for performing focusing error detection and tracking error detection of a laser beam converged on an optical disk. The optical device includes a diffraction grating having first, second, third, and fourth regions for diffracting a reflected beam from the optical disk in different directions. The optical device further includes a first photodetector for detecting a part of the reflected beam diffracted by the first region of the diffraction grating, a second photodetector for detecting a part of the reflected beam diffracted by the second region of the diffraction grating, a third photodetector for detecting a part of the reflected beam diffracted by the third region of the diffraction grating, and a fourth photodetector for detecting a part of the reflected beam diffracted by the fourth region of the diffraction grating. The shape and size of each of the first and second regions of the diffraction grating are optimally controlled to thereby increase a quantity of light incident on the photodetectors for focusing error detection.
    • 一种用于光盘驱动器的光学装置,用于执行会聚在光盘上的激光束的聚焦误差检测和跟踪误差检测。 光学装置包括具有第一,第二,第三和第四区域的衍射光栅,用于沿不同方向衍射来自光盘的反射光束。 光学装置还包括第一光电检测器,用于检测由衍射光栅的第一区域衍射的部分反射光束;第二光电检测器,用于检测由衍射光栅的第二区域衍射的部分反射光束;第三光电检测器 用于检测由衍射光栅的第三区域衍射的一部分反射光束;以及第四光电检测器,用于检测由衍射光栅的第四区域衍射的部分反射光束。 最佳地控制衍射光栅的第一和第二区域的形状和尺寸,从而增加入射到用于聚焦误差检测的光电探测器上的光量。
    • 92. 发明授权
    • Light beam scanning apparatus comprising a first and second diffraction
grating plate
    • 光束扫描装置,包括第一和第二衍射光栅板
    • US5680253A
    • 1997-10-21
    • US949520
    • 1992-11-25
    • Shinya HasegawaShigeo KayashimaSatoshi MaedaShigetake IwataFumio YamagishiMasato NakashimaHirokazu AritakeMamoru Hokari
    • Shinya HasegawaShigeo KayashimaSatoshi MaedaShigetake IwataFumio YamagishiMasato NakashimaHirokazu AritakeMamoru Hokari
    • G02B5/32G02B26/10G03H1/12G02B5/18
    • G02B5/32G02B26/106G03H1/0005
    • A high-resolution light-beam scanning apparatus utilizing only mass-producible holograms instead of utilizing auxiliary optical systems, and capable of compensating for disadvantages. The light-beam scanning apparatus including diffraction gratings for minimizing either: a sum total of values obtained by weighting a square of an optical path length difference between an optical path of a light flux measured along a principle axis of a light beam incident on and diffracted by a first diffraction grating of a rotatable hologram, and incident on and diffracted by a second diffraction grating of a fixed plate to conduct a scanning and converging on a scanning point on an image formation surface, and an optical path of a light flux measured along a marginal ray distanced from the principal axis or an absolute value of the optical path difference thereof; or a sum total of values obtained by weighting a square of a sum obtained by adding an amount of displacement of a light-beam convergent on a scanning point on the image formation surface, to an amount of displacement of the same light. The displacement measured with respect to the principal axis of a phase recorded on the diffraction grating when the light flux is incident on the fixed plate or by weighting an absolute value of the sum. The weighting is conducted at every scanning position of an image formation surface.
    • 高分辨率的光束扫描装置仅利用大量生产的全息图而不是利用辅助光学系统,并且能够补偿缺点。 该光束扫描装置包括用于最小化以下的衍射光栅:通过对沿着入射和衍射的光束的主轴测量的光通量的光路之间的光程长度差的平方加权获得的值的总和 通过可旋转全息图的第一衍射光栅,入射并由固定板的第二衍射光栅衍射,以对扫描点进行扫描和会聚,并且沿着图像形成表面测量的光通量的光路 与主轴相距的边缘光线或其光程差的绝对值; 或通过将在图像形成表面上的扫描点上收敛的光束的位移量相加而获得的和的平方加权到相同光的位移量而获得的值的总和。 当光束入射到固定板上时,相对于记录在衍射光栅上的相位的主轴测量的位移或通过加权的绝对值。 加权在图像形成表面的每个扫描位置进行。
    • 93. 发明授权
    • Optimized design method for holographic optical element and apparatus
using such holographic optical element
    • 全息光学元件的优化设计方法和使用这种全息光学元件的设备
    • US5361149A
    • 1994-11-01
    • US853624
    • 1992-03-19
    • Shinya HasegawaShigeo Kayashima
    • Shinya HasegawaShigeo Kayashima
    • B41J2/44G02B5/32G02B26/10G03H1/08
    • G02B5/32G02B26/106
    • An optimized design method of a holographic optical element by calculating a correction coefficient so that an evaluating amount of a reconstructed light reconstructed by the holographic optical element can be minimized, the correction coefficient determining an aspheric term included in a phase transfer function, the phase transfer function representing a shape of an interference fringe recorded on the holographic optical element. According to the method, the wavefront aberration is expressed via a linear function of the correction coefficient by positioning a main axis point on a characteristic evaluating surface onto which the reconstructed light is projected, so that a wavefront aberration of the reconstructed light can be minimized. Then, the correction coefficient is calculated based on the linear function so that the evaluating amount can minimized.
    • 通过计算校正系数使得由全息光学元件重建的重建光的评估量可以最小化的全息光学元件的优化设计方法,确定包括在相位传递函数中的非球面项的校正系数,相位转移 表示记录在全息光学元件上的干涉条纹的形状的功能。 根据该方法,通过将主轴点定位在其上投射有重构光的特性评估表面上,通过校正系数的线性函数来表示波前像差,从而可以使重构光的波前像差最小化。 然后,基于线性函数计算校正系数,使得评估量可以最小化。
    • 94. 发明授权
    • Method and apparatus for light beam scanning using a hologram
    • 使用全息图进行光束扫描的方法和装置
    • US4925262A
    • 1990-05-15
    • US273624
    • 1988-11-17
    • Fumio YamagishiShinya HasegawaHiroyuki Ikeda
    • Fumio YamagishiShinya HasegawaHiroyuki Ikeda
    • G06K7/12G02B5/32G02B26/10G06K15/12H04N1/113
    • G06K15/1285G02B26/106
    • A method for constructing a hologram on a transparent disk which includes two steps. First, irradiating a reference wave light beam having a diverging spherical wave front from a first point light source located at a predetermined distance on a center axis of the transparent disk. Second, irradiating an object wave light beam having a diverging spherical wave front from a second point light source located at a predetermined distance on a normal line away from a predetermined distance from the center axis. The result is interference between the reference wave light beam irradiated by the first point light source and the object wave light beam irradiated by the second point light source on the transparent disk and the formation of interference fringes having an extreme value of a spatial frequency as a hologram in one embodiment, a reconstruction beam is irradiated to the position, or in the vicinity of the extreme value.
    • 一种在透明盘上构造全息图的方法,包括两个步骤。 首先,从位于透明盘的中心轴上的预定距离的第一点光源照射具有发散的球面波前的参考波光束。 其次,从距离中心轴规定距离的法线上距预定距离的第二点光源照射具有发散球面波的物波光束。 结果是由第一点光源照射的参考波光束与由透明盘上的第二点光源照射的物体光束之间的干涉,以及具有空间频率的极值的干涉条纹的形成为 在一个实施例中,全息图将重建光束照射到极值的位置或附近。
    • 96. 发明申请
    • ELECTROMAGNETIC WAVE IMAGING APPARATUS
    • 电磁波成像装置
    • US20120120231A1
    • 2012-05-17
    • US13251670
    • 2011-10-03
    • Norihiko ItaniKazunori MaruyamaShinya Hasegawa
    • Norihiko ItaniKazunori MaruyamaShinya Hasegawa
    • H04N7/18H04N5/335
    • H04N5/30G01N21/3581G01S7/4811G01S17/89G02F1/03G02F2203/13
    • A first optical system irradiates a target with a detecting wave and making the detecting wave that is transmitted through the target incident upon the electrooptical crystal. A second optical system slants a pulse plane of a probe wave relative to a pulse plane of the detecting wave and making the probe wave incident upon the electrooptical crystal. A camera detects the probe wave passing through the electrooptical crystal. The first or second optical system includes a compensating component which partitions a beam cross section of the detecting wave or the probe wave into unit areas. The optical component makes different an optical path length of a beam passing each unit area and compensates a phase shifting between the pulse plane of the detecting wave and the pulse plane of the probe wave at positions in a crossing direction of a surface of the electrooptical crystal and the virtual plane.
    • 第一光学系统用检测波照射目标,并使通过目标传输的检测波入射到电光学晶体上。 第二光学系统相对于检测波的脉冲平面倾斜探测波的脉冲平面,并使探针波入射到电光学晶体上。 摄像机检测穿过电光晶体的探测波。 第一或第二光学系统包括将检测波或探测波的束横截面分隔成单位区域的补偿部件。 光学部件使通过每个单位面积的光束的光程长度不同,并且补偿检测波的脉冲平面与探针波的脉冲平面之间在电光水晶表面的交叉方向的位置处的相移 和虚拟平面。
    • 99. 发明申请
    • Magnetic recording medium for thermally assisted magnetic recording
    • 用于热辅助磁记录的磁记录介质
    • US20100290148A1
    • 2010-11-18
    • US12776858
    • 2010-05-10
    • Fumihiro TawaWataru OdajimaShinya Hasegawa
    • Fumihiro TawaWataru OdajimaShinya Hasegawa
    • G11B5/02G11B5/66G11B5/73
    • G11B5/667G11B5/7325G11B5/82G11B2005/0021
    • A magnetic recording medium used for the thermally assisted magnetic recording system which fires a laser beam at a magnetic recording medium to partially heat the medium and applies a magnetic field from the outside to the part heated to lower the coercivity for recording. The magnetic recording medium is configured by a glass substrate on which a heat radiation layer, heat retention layer, intermediate layer, and recording layer are stacked. Further, the heat retention layer is configured by a member having an effective refractive index lower than the effective refractive index of the recording layer and having an temperature diffusion coefficient determined by the specific heat, density, and heat conductivity rate higher than glass and lower than metal. The material with a high temperature diffusion coefficient is used lowered in temperature diffusion coefficient using a porous structure or granular structure.
    • 一种用于热辅助磁记录系统的磁记录介质,其在磁记录介质上激发激光束以部分地加热介质并将磁场从外部施加到被加热以降低用于记录的矫顽力的部分。 磁记录介质由玻璃基板构成,其上堆叠有散热层,保温层,中间层和记录层。 此外,保温层由具有低于记录层的有效折射率的有效折射率的构件构成,并且具有由比玻璃高的比热,密度和导热率确定的温度扩散系数,并且低于 金属。 使用具有高温扩散系数的材料使用多孔结构或颗粒结构降低温度扩散系数。