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
    • 3. 发明公开
    • FOURIER-DOMAIN OCT RAY-TRACING AM AUGE
    • 奥地利十字路口太空追踪
    • EP1781161A1
    • 2007-05-09
    • EP05769744.3
    • 2005-07-26
    • Carl Zeiss Meditec AG
    • FERCHER, Adolf, Friedrich
    • A61B3/107A61B3/103
    • A61B3/102A61B3/103
    • The invention relates to an ophthalmologic measuring method that can depict three-dimensional structures of the interfaces of an eye by means of low coherence interferometry based on reference points. To this end, the pupil is illuminated at a number of points by a low coherence light source (1). The measurement radiation (18) reflected at these points by the interfaces and surfaces of the eye (13) is superimposed with a reference radiation (17). The measurement data generated hereby are spectrally split up by a diffraction grating (16), projected onto a two-dimensional detector array (15), and routed to a control unit that determines a three-dimensional structure of all intraocular interfaces and surfaces of the eye (13). During the inventive Fourier domain OCT method, the depiction of the three-dimensional structures preferably ensues by means of spline surfaces or polygonal surfaces. This makes it possible to determine the depth positions of the measuring beams at many pupil points with a single image taken by the array camera by illuminating the pupil with an aperture grid, and the reference mirror contains a periodic phase grid.
    • 6. 发明公开
    • KURZKOHÄRENZ-INTERFEROMETRISCHE LÄNGENMESSUNG AM AUGE
    • 短相干干涉测量长度测量EYES ON
    • EP1713378A1
    • 2006-10-25
    • EP05726333.7
    • 2005-02-04
    • Carl Zeiss Meditec AG
    • FERCHER, Adolf, Friedrich
    • A61B3/10A61B3/12G01B9/02G01B11/14
    • A61B3/102
    • The short-coherence interferometric measurement of length on the eye has two drawbacks. First, the working focus and coherence window do not, for the most part, coincide. Second, the scanning process along the eye axis requires time. Both result in poor signal quality and inaccurate measurements. The invention provides a short-coherence interferometer, in which a 90 degree mirror and focusing optics, together, execute a periodic to-and-fro movement in such a manner that the working beam focus, which is created by the focusing optics and projected onto the eye by relay optics, is synchronously moved with the coherence window from the cornea along the optical axis of the eye to the fovea centralis. In addition, different wavelengths are, by means of a number of reflectors, generated in the working beam paths and reference beam paths whereby limiting the scanning process to distances shorter than the optical length of the eye. The invention is advantageously implemented by using a fiber-optic interferometer. The inventively designed reference interferometer arms and measuring interferometer arms are combined with the arms of a fiber-optic interferometer.
    • 10. 发明公开
    • VERFAHREN UND ANORDNUNG ZUR MESSUNG DER DISPERSION IN TRANSPARENTEN MEDIEN
    • 方法和装置,用于测量透明介质中的分散
    • EP1587415A1
    • 2005-10-26
    • EP03785827.1
    • 2003-12-16
    • Carl Zeiss Meditec AG
    • FERCHER, Adolf, Friedrich
    • A61B5/00
    • A61B5/1455A61B5/14532
    • The invention relates to methods and assemblies for measuring a dispersion and content of glucose in organic transparent and semitransparent tissues and liquids by low-coherent interference optical refractometry. Low-coherent interferometry and spectral interferometry methods are modified in such a way that a tissue thickness and local dispersion are measurable. For a technology based on low-coherent interferometry, partial interferograms received from low-coherent interferograms G (τ) are used for a dispersion measurement. For a technology based on spectral interferometry, the partial areas of a spectrum φ of a spectral interferogram are used for a dispersion measurement. The figure 6 displays an assembly based on spectral interferometry. A time-dependent low-coherent light source (1) illuminates a modified Michelson interferometer. A beam splitter (4) splits an illuminant beam into a measuring beam (5) and a reference beam (6). Light waves (46 and 6) reflected outside the interferometer reach a spectrometer at the exit of the interferometer. The recorded spectral interferogram i (φ) provides with a basis for calculating the dispersions of different waves. The viewing direction of the eye of a subject who makes said calculation is fixed by means of a target beam (32).