会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 11. 发明授权
    • Light beam scanning apparatus
    • 光束扫描装置
    • US6020999A
    • 2000-02-01
    • US838937
    • 1997-04-23
    • Shinya HasegawaShigeo KayashimaSatoshi MaedaHirokazu Aritake
    • Shinya HasegawaShigeo KayashimaSatoshi MaedaHirokazu Aritake
    • G02B5/32G02B26/10G03H1/12
    • G02B5/32G02B26/106G03H1/0005
    • A high-resolution light-beam scanning apparatus utilizing only mass-producable holograms instead of utilizing auxiliary optical systems such as optical lenses or a mirror having curvature. The light beam scanning apparatus is capable of compensating for disadvantages including scanning beam thickening and variation, failure of a rotatable hologram to rotate at a constant velocity, displacement of a scanning beam position in the scanning direction and the cross scanning direction due to a mode hop of a wavelength of a semiconductor laser, and deviation of a base of a rotatable hologram from a parallel state, which disadvantages are detrimental to efforts for increasing the resolution of a hologram scanner and lowering the cost thereof. The light beam scanning apparatus incudes at least two holograms with an optical path length difference .DELTA..PHI.
    • 仅使用可批量生产的全息图而不是使用诸如光学透镜或具有曲率的反射镜的辅助光学系统的高分辨率光束扫描装置。 光束扫描装置能够补偿扫描光束增厚和变化,可旋转全息图以恒定速度旋转的故障,扫描方向上的扫描光束位置的偏移和由于模式跳跃而产生的横向扫描方向的缺点 半导体激光器的波长以及可旋转全息图的基底与平行状态的偏差,这些缺点对于增加全息扫描仪的分辨率和降低其成本的努力是有害的。 光束扫描装置包含光路长度差DELTA PHI <(λ2 / Dλ)的至少两个全息图,其中<常数小于0.5。 路径长度根据上述方程与在光表面的中心处的波长λ相关,并且在光表面的中心处从波长+558测量的波长位移DELTAλλ。
    • 13. 发明授权
    • Light beam scanning apparatus
    • 光束扫描装置
    • US6040929A
    • 2000-03-21
    • US844994
    • 1997-04-23
    • Shinya HasegawaShigeo KayashimaSatoshi MaedaHirokazu Aritake
    • Shinya HasegawaShigeo KayashimaSatoshi MaedaHirokazu Aritake
    • G02B5/32G02B26/10G03H1/12G02B27/44
    • G02B5/32G02B26/106G03H1/0005
    • A high-resolution light-beam scanning apparatus utilizing only mass-producible holograms instead of utilizing auxiliary optical systems such as optical lenses or a mirror having curvature, and capable of compensating for disadvantages including scanning beam thickening and variation, failure of a rotatable hologram to rotate at a constant velocity, displacement of a scanning beam position in the scanning direction and the cross scanning direction due to a mode hop of a wavelength of a semiconductor laser, and deviation of a base of rotatable hologram from a parallel state. These disadvantages are detrimental to efforts for increasing the resolution of a hologram scanner and lowering the cost thereof. The light beam scanning apparatus includes at least two holograms, one rotatable and one fixed, wherein the fixed hologram plate has a phase distribution .PHI..sub.H represented as a difference obtained when subtracting a reference wave phase .PHI..sub.0 from an object wave phase .PHI..sub.R, where X is a scanning direction and Y is a cross scanning direction, C.sub.0, C.sub.1, C.sub.2, Y.sub.0, and Z.sub.0 are constants, where .lambda..sub.2 is a wavelength of said incident light; and .lambda..sub.1 is a wavelength of a constructing wave used for forming said fixed hologram plate.
    • 仅利用大规模生产的全息图的高分辨率光束扫描装置,而不是利用诸如光学透镜或具有曲率的反射镜等辅助光学系统,并且能够补偿包括扫描光束增厚和变化的缺点,可旋转全息图的故障 以恒定速度旋转,由于半导体激光器的波长的模式跳跃而导致的扫描光束位置在扫描方向和横扫描方向上的位移以及可旋转全息图的基底与平行状态的偏离。 这些缺点对于增加全息扫描仪的分辨率并降低其成本的努力是有害的。 光束扫描装置包括至少两个可旋转和一个固定的全息图,其中固定全息图板具有相位分布PHI H,该相位分布PHI H表示为从对象波相位PHI R减去参考波相位PHI 0时获得的差值,其中 X是扫描方向,Y是交叉扫描方向,C0,C1,C2,Y0和Z0是常数,其中λ2是所述入射光的波长; λ1是用于形成所述固定全息图板的构造波的波长。
    • 16. 发明授权
    • Light beam scanning apparatus
    • 光束扫描装置
    • US5940195A
    • 1999-08-17
    • US847317
    • 1997-04-23
    • Shinya HasegawaFumio YamagishiMasato Nakashima
    • Shinya HasegawaFumio YamagishiMasato Nakashima
    • G02B5/32G02B26/10G03H1/12
    • G02B5/32G02B26/106G03H1/0005
    • A high-resolution light-beam scanning apparatus utilizing only mass-producible holograms instead of utilizing auxiliary optical systems such as optical lenses or a mirror having curvature, and capable of compensating for disadvantages including scanning beam thickening and variation, failure of a rotatable hologram to rotate at a constant velocity, displacement of a scanning beam position in the scanning direction and the cross scanning direction due to a mode hop of a wavelength of a semiconductor laser, and deviation of a base of rotatable hologram from a parallel state. These disadvantages are detrimental to efforts for increasing the resolution of a hologram scanner and lowering the cost thereof. The light beam scanning apparatus includes at least two holograms with an optical path length difference .DELTA..PHI. along a scanning beam light flux. The path length is measured from a light source to a scanning surface in the first hologram, and is represented by .DELTA..PHI.
    • 仅利用大规模生产的全息图的高分辨率光束扫描装置,而不是利用诸如光学透镜或具有曲率的反射镜等辅助光学系统,并且能够补偿包括扫描光束增厚和变化的缺点,可旋转全息图的故障 以恒定速度旋转,由于半导体激光器的波长的模式跳跃而导致的扫描光束位置在扫描方向和横扫描方向上的位移以及可旋转全息图的基底与平行状态的偏离。 这些缺点对于增加全息扫描仪的分辨率并降低其成本的努力是有害的。 光束扫描装置沿扫描光束光束包括至少两个具有光程长度差DELTA PHI的全息图。 路径长度从第一全息图中的光源到扫描面测量,并由DELTA PHI
    • 17. 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。
    • 20. 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。