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    • 1. 发明申请
    • Method and System for Optical Coherence Tomography
    • 光学相干断层扫描的方法和系统
    • US20140218740A1
    • 2014-08-07
    • US14009363
    • 2012-03-30
    • Rainer NebosisGeert Wellens
    • Rainer NebosisGeert Wellens
    • G01B9/02
    • G01B9/02091A61B5/0066A61B2560/0437G01B9/02063G01B9/02085G01B9/02089G01N21/4795
    • The present invention relates to a method as well as a corresponding system (50) for optical coherence tomography in which a first image (60) is acquired in the region of a first plane of an object (1) by means of an optical coherence tomography equipment, and the first image (60) is displayed on a display device (52).To facilitate a reliable and time-saving examination with straightforward handling, provision is made that a second plane of the object (1) is selected on the basis of the first image (60) that is displayed on the display device (52), wherein the second plane of the object (1) is different from the first plane of the object (1), and a second image (61) is acquired in the region of the selected second plane of the object (1) by means of the optical coherence tomography equipment.
    • 本发明涉及一种用于光学相干断层摄影的相应系统(50),其中通过光学相干断层扫描在物体(1)的第一平面的区域中获取第一图像(60) 设备,并且第一图像(60)被显示在显示设备(52)上。 为了便于直接处理的可靠且省时的检查,提供了基于显示在显示装置(52)上的第一图像(60)选择对象(1)的第二平面,其中, 物体(1)的第二平面不同于物体(1)的第一平面,并且在物体(1)的所选择的第二平面的区域中通过光学器件(1)获取第二图像(61) 相干层析成像设备。
    • 3. 发明申请
    • Method and System for Optical Coherence Tomography
    • 光学相干断层扫描的方法和系统
    • US20140204391A1
    • 2014-07-24
    • US14009371
    • 2012-03-30
    • Rainer NebosisGeert WellensWolfgang Schorre
    • Rainer NebosisGeert WellensWolfgang Schorre
    • G01B9/02
    • G01B9/02089A61B5/0066A61B5/0073A61B5/444A61B2560/0437A61B2562/0233G01B9/02063G01B9/02091G01N21/4795G06T2219/028
    • The present invention relates to a method as well as a corresponding system (50) for optical coherence tomography, where, by means of an optical coherence tomography equipment, a first image (60) is acquired in the region of a first plane of an object (1) and a second image (61) is acquired in the region of a second plane of the object (1), wherein the second plane of the object (1) is different from the first plane of the object (1).To facilitate a reliable and time-saving examination of the object (1), with the most straightforward handling possible, the first image (60) is acquired in the region of the first plane (S) of the object (1) and the second image (61) is acquired in the region of the second plane (F) of the object (1) in real time, and the first image (60) or the second image (61) is rendered as a real time image and the respectively other image, i.e. the second or the first image (61 or 60 respectively), is rendered as a still image on the display device (52) depending on a control command, in particular one entered by an operator.
    • 本发明涉及一种用于光学相干断层摄影的方法以及相应的系统(50),其中通过光学相干断层摄影设备,在物体的第一平面的区域中获取第一图像(60) (1)和第二图像(61)在对象(1)的第二平面的区域中获取,其中对象(1)的第二平面不同于对象(1)的第一平面。 为了便于对物体(1)的可靠和省时的检查,以最直接的处理可能,在物体(1)的第一平面(S)的区域中获取第一图像(60),第二图像 实时地在物体(1)的第二平面(F)的区域中获取图像(61),并且将第一图像(60)或第二图像(61)分别呈现为实时图像,并且分别 其他图像,即第二图像或第一图像(分别为61或60)根据控制命令,特别是由操作者输入的控制命令,在显示装置(52)上呈现为静止图像。
    • 4. 发明申请
    • System and Method for Optical Coherence Tomography and Method for Calibrating Said Type of System
    • 用于光学相干断层扫描的系统和方法以及校准所述系统类型的方法
    • US20100027029A1
    • 2010-02-04
    • US12527292
    • 2008-02-20
    • Rainer NebosisRainer ScheunemannEdgar-Gerald Kopp
    • Rainer NebosisRainer ScheunemannEdgar-Gerald Kopp
    • G01B11/14
    • G01B9/02091G01B9/02002G01B9/02012G01B9/02063G01B9/02072
    • The invention relates to a system and to a corresponding method for optical coherence tomography having an interferometer (10) for emitting light with which a specimen (1) is irradiated, the interferometer (1) comprising a beam splitter (13) and at least one reflector (12) the optical distance (I) of which from the beam splitter (13) is changeable, a specimen objective by means of which light emitted by the interferometer (10) is focussed in a focus lying within the specimen (1), and a detector (30) for collecting light which is reflected by the specimen (1).For simpler and quicker recording of the sharpest possible images of the specimen (1) provision is made such that during a change of the optical distance (I) between the reflector (12) and the beam splitter (13) the light respectively reflected at a number of different depths of the specimen (1) is collected by the detector (30), and during the collection of the light respectively reflected at the different depths of the specimen (1) the imaging properties of the specimen objective are changed such that the focus comes within the range of the respective depth of the specimen (1).
    • 本发明涉及一种用于光学相干断层摄影的系统和相应的方法,该方法具有用于发射照射样本(1)的光的干涉仪(10),所述干涉仪(1)包括分束器(13)和至少一个 反射器(12),来自分束器(13)的光学距离(I)可以改变,由干涉仪(10)发射的光聚焦在位于样品(1)内的焦点上的样本物镜, 以及用于收集被样品(1)反射的光的检测器(30)。 为了更简单和更快速地记录样本的最清晰可能的图像(1),提供这样的设置,使得在反射器(12)和分束器(13)之间的光学距离(I)的改变期间,分别在一个 样品(1)的不同深度的数量由检测器(30)收集,并且在分别在样品(1)的不同深度处反射的光的收集期间,改变样品物镜的成像特性,使得 焦点在样本(1)的相应深度的范围内。
    • 7. 发明授权
    • System and method for optical coherence tomography
    • 光学相干断层扫描系统和方法
    • US08810797B2
    • 2014-08-19
    • US12527287
    • 2008-02-20
    • Rainer NebosisRainer ScheunemannEdgar-Gerald Kopp
    • Rainer NebosisRainer ScheunemannEdgar-Gerald Kopp
    • G01B11/02
    • G01B9/02012G01B9/02002G01B9/02063G01B9/02071G01B9/02072G01B9/02091
    • The invention relates to a system and to a corresponding method for optical coherence tomography having an interferometer (10) for emitting light with which a specimen (1) is irradiated, the interferometer (1) comprising a beam splitter (13) and at least one reflector (12) the optical distance (I) of which from the beam splitter (13) is changeable, and a detector (30) which has a plurality of detector elements arranged in an area by means of which the light which is reflected by the specimen (1) is collected.In order to simplify and speed up the recording of three-dimensional images of the specimen (1) provision is made such that the optical distance (I) between the reflector (12) and the beam splitter (13) is changed by an optical path (L) which is substantially greater than an average wavelength (λ0) of light (14) which is injected into the interferometer (10): L>>λ0, during the change of the optical distance (I) between the reflector (12) and the beam splitter (13) by the optical path (L) the light reflected by the specimen (1) being collected a number of times by the detector elements of the detector (30), by means of which the light reflected by a number of two-dimensional sections at different depths of the specimen (1) is collected.
    • 本发明涉及一种用于光学相干断层摄影的系统和相应的方法,该方法具有用于发射照射样本(1)的光的干涉仪(10),所述干涉仪(1)包括分束器(13)和至少一个 反射器(12),来自分束器(13)的光学距离(I)可以改变;以及检测器(30),其具有多个检测器元件,所述检测器元件布置在通过该区域反射的光的区域中, 收集样品(1)。 为了简化和加快样本的三维图像的记录(1),提供反射器(12)和分束器(13)之间的光学距离(I)由光路 (L),其在反射器(12)之间的光学距离(I)的改变期间基本上大于注入到干涉仪(10)中的光(14)的平均波长(λ0):L >>λ0 并且通过光路(L)的分束器(13)被检体(1)反射的光被检测器(30)的检测器元件收集多次,通过该检测器元件反射数量 收集样品(1)不同深度的二维截面。
    • 8. 发明授权
    • System and method for optical coherence tomography with light or detector modulation
    • 具有光或检测器调制的光学相干断层扫描的系统和方法
    • US08593639B2
    • 2013-11-26
    • US12527322
    • 2008-02-20
    • Rainer Nebosis
    • Rainer Nebosis
    • G01B11/02
    • G01B9/02091A61B5/0066A61B5/0073A61B5/444G01B9/02002G01B9/02012G01B9/02063G01B9/02072G01N21/4785G01N21/4795G01N2021/4709
    • The invention relates to a system and to a corresponding method for optical coherence tomography having an interferometer (10) for emitting light with which a specimen (1) is irradiated, the interferometer (10) comprising a beam splitter (13) and at least one reflector (12) the optical distance (I) of which from the beam splitter (13) can be changed by an optical path (L), and a detector (30) with a first number of detector elements arranged in a first area for collecting light which is reflected by the specimen (1).In order to be able to record images of a specimen, in particular in real time, more simply and quickly, the system is operated in a first mode in which light reflected by the specimen (1) is only collected by a second number of detector elements of the detector (30) and converted into corresponding detector signals, the second number of detector elements being smaller than the first number of detector elements.
    • 本发明涉及一种用于光学相干断层摄影的系统和相应的方法,该方法具有用于发射照射样本(1)的光的干涉仪(10),所述干涉仪(10)包括分束器(13)和至少一个 反射器(12)可以通过光路(L)改变来自分束器(13)的光学距离(I),以及具有第一数量的检测器元件的检测器(30),其布置在第一区域中用于收集 由样品(1)反射的光。 为了能够更简单快速地记录样本的图像,特别是实时地,快速地记录图像,其中由样本(1)反射的光仅由第二数量的检测器收集的第一模式操作 检测器(30)的元件并转换成对应的检测器信号,第二数量的检测器元件小于第一数量的检测器元件。
    • 10. 发明申请
    • System and Method for Optical Coherence Tomography
    • 光学相干断层扫描的系统和方法
    • US20100033726A1
    • 2010-02-11
    • US12527298
    • 2008-02-20
    • Rainer NebosisRainer Scheunemann
    • Rainer NebosisRainer Scheunemann
    • G01B9/02
    • G01B9/02012G01B9/02002G01B9/02063G01B9/02072G01B9/02091
    • The invention relates to a system and to a corresponding method for optical coherence tomography having an interferometer (10) which has a beam splitter (13), a first reflector (11) and a reflector (12) the optical distance (I) of which from the beam splitter (13) is changeable by a speed (v), and a detector (30) for collecting light which is reflected by a specimen (1) to be examined.In order to reduce the times required for the most reliable possible recording of interference patterns, provision is made such that the intensity of the light (14 or 4) injected into the interferometer (10) or emitted by the interferometer (10) is modulated with a modulation frequency (fM) which is not equal to the Doppler frequency (fD), the Doppler frequency (fD) being given by twice the ratio of the speed (v) of the change of the optical distance (I) between the reflector (12) and the beam splitter (13) to the average wavelength (λ0) of the injected light (14): fM≠fD=2·v/λ0.
    • 本发明涉及一种具有干涉仪(10)的光学相干断层摄影的系统和相应方法,所述干涉仪具有分束器(13),第一反射器(11)和反射器(12),光学距离(I) 来自分束器(13)的速度可以通过速度(v)变化;以及检测器(30),用于收集被检查样本(1)反射的光。 为了减少最可靠地记录干涉图案所需的时间,提供这样的设置,使得注入干涉仪(10)或由干涉仪(10)发射的光(14或4)的强度用 不等于多普勒频率(fD)的调制频率(fM),多普勒频率(fD)由反射器(1)之间的光学距离(I)的变化的速度(v) 12)和分束器(13)到注入的光(14)的平均波长(λ0):fMfD = 2.v /λ0。