Ink regulation device for a printing machine
    131.
    发明申请
    Ink regulation device for a printing machine 有权
    印刷机油墨调节装置

    公开(公告)号:US20010010191A1

    公开(公告)日:2001-08-02

    申请号:US09805086

    申请日:2001-03-13

    CPC classification number: G01J3/46 B41F33/0045 G01J3/0224 G01J3/463 G01J3/502

    Abstract: An ink regulating device that measures color in a web-fed rotary printing machine for printing a printing material web or sheets in a plurality of colors. The ink regulating device measures and evaluates the colors black, cyan, magenta, and yellow, and after general calibration (i.e., the recording of standard values), derives set values for the inking zone setting devices, without requiring any further patterns, and without the need for a special copy when the printing pattern is changed.

    Abstract translation: 一种油墨调节装置,用于测量卷筒纸式旋转印刷机中用于印刷多种颜色的印刷材料幅材或纸张的颜色。 墨水调节装置测量和评估黑色,青色,品红色和黄色的颜色,并且在通常校准(即标准值的记录)后)导出着墨区域设置装置的设定值,而不需要任何进一步的图案,并且没有 当打印图案改变时,需要特殊的复印件。

    Interferometer and methods for compensation of dispersion or increase in spectral resolution of such an interferometer
    132.
    发明授权
    Interferometer and methods for compensation of dispersion or increase in spectral resolution of such an interferometer 失效
    用于补偿这种干涉仪的色散或增加光谱分辨率的干涉仪和方法

    公开(公告)号:US06249350B1

    公开(公告)日:2001-06-19

    申请号:US09242005

    申请日:1999-12-09

    Abstract: A double-beam interferometer for electromagnetic radiation and a method for the compensation of dispersion or increase in the spectral resolution of such an interferometer. Using a polarizer, which is brought into the optical radiation path, a defined polarization state P½0 is produced for the electromagnetic partial waves flowing into the arms of the interferometer. This polarization state is wavelength-independent and can vary for both partial beams. Optical elements modify the polarization state P½0 of the electromagnetic partial waves as a function of wavelength &lgr; and each spectral component &lgr;i is coded with a polarization P½ (&lgr;i). An analyzer, fitted to the output of the interferometer, transmits an adjustable polarization state Pdet, whereby an additional wavelength-dependent phase difference &ggr;(&lgr;) occurs between the partial waves of the spectral components. &ggr;(&lgr;) can be adjusted to obtain compensation of dispersion or an increase in the spectral resolution of the interferometer.

    Abstract translation: 用于电磁辐射的双光束干涉仪和用于补偿这种干涉仪的色散或增加光谱分辨率的方法。 使用入射到光学辐射路径中的偏振器,对于流入干涉仪的臂的电磁分波产生限定的偏振状态P 1/2。 该偏振状态是波长无关的,并且对于两个部分光束可以变化。 光学元件将电磁分波的偏振状态P 1/2作为波长的函数进行修改,并且以偏振P 1/2(兰德)编码每个光谱分量lambdi。 安装在干涉仪的输出端的分析仪透射可调极化状态Pdet,由此在光谱分量的部分波之间产生附加的波长相关的相位差γ(lambd)。 可以调整伽马(羔羊)以获得色散的补偿或干涉仪的光谱分辨率的增加。

    Low insertion loss optical monochromator
    133.
    发明授权
    Low insertion loss optical monochromator 失效
    低插入损耗光学单色仪

    公开(公告)号:US06177992B1

    公开(公告)日:2001-01-23

    申请号:US09160650

    申请日:1998-09-25

    CPC classification number: G01J3/02 G01J3/0224 G01J3/12 G01J3/447

    Abstract: An optical monochromator has high signal selectivity and low insertion loss, and is well-suited for characterizing a variety of optical signals, including closely-spaced optical channels within DWDM systems. The optical monochromator includes a bulk-optic polarization beam splitter that separates orthogonal polarization states of an applied optical signal into separate optical beams. Low insertion loss is achieved by reconciling the polarization states of the separate optical beams to an optimum polarization state that minimizes insertion loss when the optical beams are applied to a dispersive element. High signal selectivity is achieved using a multipass configuration and by illuminating large areas of the dispersive element, since large beam diameters are accommodated by the bulk-optic polarization beam splitter.

    Abstract translation: 光学单色仪具有高信号选择性和低插入损耗,并且非常适用于表征各种光信号,包括DWDM系统内的紧密间隔的光通道。 光学单色仪包括将所施加的光信号的正交偏振状态分离为单独的光束的体光学偏振分束器。 通过将分离的光束的偏振状态协调到当将光束施加到色散元件时使插入损耗最小化的最佳偏振状态来实现低插入损耗。 通过使用多通道配置和照亮大面积的色散元件实现高信号选择性,因为大光束直径由体光学偏振分束器容纳。

    Method and an apparatus for determining the color stimulus specification
of an object
    134.
    发明授权
    Method and an apparatus for determining the color stimulus specification of an object 有权
    用于确定对象的颜色刺激规格的方法和装置

    公开(公告)号:US6038024A

    公开(公告)日:2000-03-14

    申请号:US227666

    申请日:1999-01-08

    Applicant: Markus Berner

    Inventor: Markus Berner

    Abstract: In order to determine the color stimulus specification of a translucent object under test, it is suggested to illuminate the object under test with light having different wave length bandwidth portions, or, alternatively, to subdivide the light reflected by the object under test into different wave length bandwidth portions before it is captured by an image sensor. To exactly approach a probe head to the object under test, the object under test is visualized with the help of a further image sensor. Preferably, two image sensors are used, whereby the one image sensor is used for visualizing the object under test and the other image sensor is used for determining the colorimetric data of the object under test. In this way, the color stimulus specification of the object under test can be determined very exactly. Moreover, such a method including an apparatus suitable for performing the method can be practically realized very easily.

    Abstract translation: 为了确定测试中的半透明物体的颜色刺激规格,建议用具有不同波长带宽部分的光照亮待测物体,或者将被测物体反射的光细分成不同的波 长度带宽部分在被图像传感器捕获之前。 为了准确地将探头接近待测物体,借助于另外的图像传感器可视化被测物体。 优选地,使用两个图像传感器,由此使用一个图像传感器来可视化待测对象,并且另一图像传感器用于确定被测物体的比色数据。 以这种方式,可以非常精确地确定被测物体的颜色刺激规格。 此外,包括适于执行该方法的装置的这种方法可以非常容易地实现。

    Means and method for measuring absorption of radiation-scattering samples
    135.
    发明授权
    Means and method for measuring absorption of radiation-scattering samples 失效
    测量辐射散射样品吸收的方法和方法

    公开(公告)号:US5963335A

    公开(公告)日:1999-10-05

    申请号:US103782

    申请日:1998-06-24

    CPC classification number: G01N21/47 G01J3/4412 G01N21/59 G01J3/0224 G01J3/0229

    Abstract: The present invention provides methods and devices for measuring radiation absorption by a sample. The invention enables one to determine whether the sample scatters the radiation of interest and, if so, to factor out the effects of such scattering and ore accurately determine the true absorption of the sample. The invention may employ a selectively controllable occluder which is moved between three or more different positions to yield three or more different radiation measurements. These measurements can then be compared to one another to determine the nature of any radiation scattering and factor out its effects, enabling more accurate absorption determinations.

    Abstract translation: 本发明提供了用于测量样品的辐射吸收的方法和装置。 本发明使得能够确定样品是否散射感兴趣的辐射,如果是这样,则排除这种散射和矿石的影响,以精确地确定样品的真实吸收。 本发明可以采用在三个或更多个不同位置之间移动的可选择性控制的闭塞器,以产生三个或更多个不同的辐射测量。 然后可以将这些测量值彼此进行比较,以确定任何辐射散射的性质并排除其影响,从而实现更准确的吸收测定。

    Interferometric acousto-optic spectrum analyzer
    136.
    发明授权
    Interferometric acousto-optic spectrum analyzer 失效
    干涉声光谱分析仪

    公开(公告)号:US5002395A

    公开(公告)日:1991-03-26

    申请号:US305196

    申请日:1989-02-02

    Applicant: Manhar L. Shah

    Inventor: Manhar L. Shah

    Abstract: An interferometric spectrum analyzer employs a pair of Bragg cells arranged in an optically cascaded configuration such that both the signal beam and the reference beam travel along a common optical path. The beam-modifying properties of the Bragg cells are such that within a prescribed bandwidth of operation, the deflection properties of the respective cells are frequency complementary, namely different frequencies applied to the respective cells deflect the beam passing therethrough along the same optical path, to produce a beat frequency at the Fourier transform plane. In accordance with a first embodiment, complementary deflection action is achieved by using Bragg cells having respectively different acoustic velocites. In a second embodiment, each Bragg cell has the same acoustic velocity. The deflection/frequency complementary effect is obtained by the use of a birefringent material prism interposed between the Bragg cells, which produces angular deviation that depends upon the polarization and the direction of propagation of light passing through the prism.

    Abstract translation: 干涉测量频谱分析仪采用布置在光级联配置中的一对布拉格单元,使得信号光束和参考光束沿着公共光路传播。 布拉格单元的波束修正特性使得在规定的操作带宽内,各个单元的偏转特性是频率互补的,即施加到各个单元的不同频率将沿着相同光路偏转的光束偏转到 在傅立叶变换平面产生拍频。 根据第一实施例,通过使用具有不同声速的布拉格电池来实现互补偏转动作。 在第二实施例中,每个布拉格单元具有相同的声速。 偏转/频率互补效应通过使用插入在布拉格单元之间的双折射材料棱镜获得,其产生取决于通过棱镜的光的偏振和传播方向的角度偏差。

    Manual device for the detection of optical reflection properties
    137.
    发明授权
    Manual device for the detection of optical reflection properties 失效
    用于检测光学反射特性的手动装置

    公开(公告)号:US4961646A

    公开(公告)日:1990-10-09

    申请号:US300929

    申请日:1989-01-24

    Abstract: A manual device for the detection of photometric data which includes a measuring head to illuminate a measuring surface and to detect the light reflected. The measuring light captured by the measuring head is spectrally decomposed by a monochromator containing a diffraction grating. The intensity of the light exiting through an outlet diaphragm is detected by a photodetector. The spectral position of the measuring light is set by a drive motor rotating a grating shaft connected with the holder of the diffraction grating. From the spectra detected, densitometric and colorimetric data are calculated by a computer, which together with the spectra determined, may be displayed on a display field.

    Abstract translation: 一种用于检测测光数据的手动装置,其包括测量头以照亮测量表面并检测反射的光。 由测量头捕获的测量光由包含衍射光栅的单色仪进行光谱分解。 通过出口隔膜排出的光的强度由光检测器检测。 测量光的光谱位置由旋转与衍射光栅的支架连接的光栅轴的驱动电机设定。 从所检测的光谱中,通过计算机计算密度和比色数据,其与确定的光谱一起可以显示在显示区域上。

    Color detection device
    138.
    发明授权
    Color detection device 失效
    颜色检测装置

    公开(公告)号:US4120591A

    公开(公告)日:1978-10-17

    申请号:US746626

    申请日:1976-12-01

    CPC classification number: G01J3/51 B07C5/342 G01J3/0224

    Abstract: Color detection apparatus wherein only light that has been diffuse-reflected, and has not been mirror-reflected, from the object whose color is to be detected is processed. Light from a source passes through a first polarizer before the light is incident on the object whose color is to be detected. Light reflected from this target object passes through a second polarizer which blocks all mirror-reflected light while permitting a portion of the diffuse-reflected light to pass. After passing through the second polarizer a portion of the light is directed onto a color filter after which the intensity of the transmitted light is detected. The intensity of the portion of light not applied to the color filter is also detected. The ratio of the output of the two detectors is a function of the color of the reflected light. The principal axis of the light incident on the target object is coincident with the principal axis of the reflected light that is to be processed, thus eliminating the need to accurately position the target object.

    Abstract translation: 处理仅从被检色对象漫反射而没有被镜面反射的光的颜色检测装置。 在光入射到要检测其颜色的物体上之前,源的光穿过第一偏振器。 从该目标物体反射的光通过第二偏振器,该第二偏振器阻挡所有镜面反射光,同时允许漫反射光的一部分通过。 在通过第二偏振器之后,将光的一部分引导到滤色器上,之后检测透射光的强度。 还检测到未施加到滤色器的光的部分的强度。 两个检测器的输出的比率是反射光的颜色的函数。 入射到目标物体上的光的主轴与要处理的反射光的主轴重合,因此不需要精确地定位目标物体。

    Monolithic optical retarder
    140.
    发明授权

    公开(公告)号:US11906770B2

    公开(公告)日:2024-02-20

    申请号:US17541037

    申请日:2021-12-02

    CPC classification number: G02B5/3091 G01J3/0224 G01J3/14 G02B5/04 G02B17/04

    Abstract: A monolithic optical retarder formed from a monolithic prism may include an input face for receiving a light beam, an output face aligned with an optical axis of the light beam prior to entering the input face, and three or more reflection faces. The three or more reflection faces may be oriented to provide an optical path for the light beam from the input face to the output face via reflection by the three or more reflection faces, where the monolithic optical retarder imparts a selected optical retardation on the light beam based on total internal reflection on at least one of the reflection faces. Further, the input face, the output face, and the three or more reflection faces may be oriented such that an optical axis of the light beam exiting the output face is equal to the optical axis of the light beam entering the input face.

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