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    • 21. 发明授权
    • Short coherence interferometry for measuring distances
    • 用于测量距离的短相干干涉测量
    • US09155462B2
    • 2015-10-13
    • US13000276
    • 2009-06-12
    • Martin HackerRalf EbersbachThomas Pabst
    • Martin HackerRalf EbersbachThomas Pabst
    • G01B9/02G01J5/60G01J3/45G01B11/02A61B3/10A61B3/15
    • A61B3/1005A61B3/102A61B3/15G01B9/02079G01B9/02091G01B9/02097G01B2290/70
    • A short coherence interferometer for measuring several axially spaced-apart regions of a sample, especially of an eye, which has a measuring optical path, through which the measuring radiation falls on the sample, a tunable interferometer for the axial, relative retardation of parts of the radiation, wherein the axial relative retardation is assigned to the axial spacing of the regions and a detector for producing an interference signal from interfering measurement radiation, scattered or reflected back from the sample as sample radiation. The tunable interferometer divides the sample radiation into two parts, which are axially relatively retarded and superimposed so as to interfere. During the superimposition, the tunable interferometer forms individual radiations, which represent quadrature components of the sample radiation, and the detector detects the individual radiations.
    • 一种用于测量样品,特别是眼睛的几个轴向间隔开的区域的短相干干涉仪,其具有测量光路,测量辐射通过该测量光路落在样品上,用于轴向相对延迟的可调干涉仪 辐射,其中轴向相对延迟被分配给区域的轴向间隔,以及用于产生来自干扰测量辐射的干扰信号的检测器,其作为样品辐射从样品散射或反射回来。 可调谐干涉仪将样本辐射分为两部分,这两部分轴向相对延迟并叠加以便干扰。 在叠加期间,可调谐干涉仪形成单个辐射,其表示样品辐射的正交分量,并且检测器检测各个辐射。
    • 26. 发明申请
    • SHORT COHERENCE INTERFEROMETER
    • 短路干扰仪
    • US20100284021A1
    • 2010-11-11
    • US12680722
    • 2008-09-26
    • Martin Hacker
    • Martin Hacker
    • G01B9/02
    • G01B9/02028A61B3/1005A61B3/102A61B3/113G01B9/02021G01B9/02035G01B9/02081G01B9/02091G01B2290/45G01B2290/70G01N21/4795G01N2021/1787
    • A short coherence interferometer apparatus for measuring multiple axially spaced regions of a specimen, in particular the eye, which has at least one measuring beam path, through which multiple individual measuring beams are incident on the specimen, and one reference beam path, through which a reference beam runs, with which the individual measuring beams are superimposed and brought into interference. The individual measuring beams are axially offset to one another upon incidence on the specimen by an amount which is adapted to the axial spacing. The interferometer apparatus superimposes each individual measuring beam with the reference beam in an interfering manner and conducts it to a detector associated with the particular individual measuring beam. The individual measuring beams are combined into a mixture in which they have varying phasing in the superposition with the reference beam.
    • 一种用于测量样本,特别是眼睛的多个轴向间隔的区域的短相干干涉仪装置,其具有至少一个测量光束路径,多个单独的测量光束通过该光束路径入射在样本上,以及一个参考光束路径, 参考光束运行,各个测量光束通过它们叠加并引起干扰。 当在试样上入射适当于轴向间距的量时,各个测量光轴彼此轴向偏移。 干涉仪装置以干扰的方式将每个单独的测量光束与参考光束重叠,并将其传导到与特定的各个测量光束相关联的检测器。 单独的测量光束被组合成混合物,在该混合物中它们与参考光束叠加时具有变化的相位。
    • 28. 发明授权
    • Method and arrangement for selecting an IOL and/or the surgical parameters within the framework of the IOL implantation on the eye
    • 用于在IOL植入眼睛框架内选择IOL和/或手术参数的方法和装置
    • US08857443B2
    • 2014-10-14
    • US13483938
    • 2012-05-30
    • Martin HackerMartin KuehnerRico FuchsMatthias Reich
    • Martin HackerMartin KuehnerRico FuchsMatthias Reich
    • A61B19/00
    • A61B3/0025A61B2034/108A61F2/1613G06F19/00G16H50/50
    • Selection of an appropriate intraocular lens (IOL) and/or the applicable surgical parameters for optimizing the results of refractive procedures on the eye. Features of the IOL are crucial for the selection and/or adjustment of the optimal IOL, but so is the IOL selection method (and parameters) from a surgical perspective. For the method, corresponding output parameters are determined from predetermined, estimated, or measured input parameters and/or their mean values, wherein at least two input parameters are varied with one another and which have at least one input parameter as a distribution function. The resulting function is optimized by means of corresponding target values and the determined distribution function of one or more output parameters is used as a decision aid. The present solution is used for selecting an appropriate IOL and/or the applicable surgical parameters and is applicable in the field of eye surgery for implanting IOLs.
    • 选择适当的眼内晶状体(IOL)和/或用于优化眼睛屈光程序结果的适用手术参数。 IOL的特征对于最佳IOL的选择和/或调整至关重要,而从手术角度来说,IOL选择方法(和参数)也是至关重要的。 对于该方法,相应的输出参数由预定的,估计的或测量的输入参数和/或它们的平均值确定,其中至少两个输入参数彼此变化并且具有至少一个输入参数作为分布函数。 所得到的函数通过相应的目标值进行优化,并且将一个或多个输出参数的确定的分布函数用作决策辅助。 本解决方案用于选择适当的IOL和/或适用的外科手术参数,并且可用于眼部手术植入IOL的领域。
    • 30. 发明申请
    • OPTIMIZED DEVICE FOR SWEPT SOURCE OPTICAL COHERENCE DOMAIN REFLECTOMETRY AND TOMOGRAPHY
    • 用于切割源的优化设备光学相关域反射光谱法和TOMOGRAPHY
    • US20130308097A1
    • 2013-11-21
    • US13981688
    • 2012-01-30
    • Ralf EbersbachMartin Hacker
    • Ralf EbersbachMartin Hacker
    • A61B3/10
    • A61B3/102G01B9/02004G01B9/02059G01B9/02091
    • Optimized device for swept source optical coherence domain reflectometry and tomography. In the coherence-optical device, light, with the aid of an interferometer, is used for distance-measuring and imaging purposes on reflecting and scattering areas of the human eye. The optimized device according to the invention consists of includes a tunable light source, matched to the sought-after measurement region ZOCT, with a resonator length LR, an interferometric measurement arrangement, a data capturing unit for capturing the light portions scattered back from the sample and a data processing unit. Here the resonator length LR of the tunable light source is matched not only to the sought-after measurement region ZOCT, but also to the entire interferometric measurement arrangement such that disturbance points present in the interferometric measurement arrangement cannot create disturbance signals in the sought-after measurement region ZOCT.
    • 扫频源光学相干域反射和层析成像的优化设备。 在相干光学装置中,借助于干涉仪的光被用于在人眼的反射和散射区域上的距离测量和成像目的。 根据本发明的优化装置包括与所寻找的测量区域ZOCT匹配的可调谐光源,具有谐振器长度LR,干涉测量装置,用于捕获从样品散射回来的光部分的数据捕获单元 和数据处理单元。 这里,可调谐光源的谐振器长度LR不仅与所寻求的测量区域ZOCT匹配,而且与整个干涉测量装置相匹配,使得存在于干涉测量装置中的干扰点不能产生所寻求的干扰信号 测量区域ZOCT。