Biological tissue analysis by inverse spectroscopic optical coherence tomography

    公开(公告)号:US09678007B2

    公开(公告)日:2017-06-13

    申请号:US13651196

    申请日:2012-10-12

    Inventor: Vadim Backman Ji Yi

    CPC classification number: G01N21/4795 A61B5/0066

    Abstract: A method and system to measure and image the full optical scattering properties by inverse spectroscopic optical coherence tomography (ISOCT) is disclosed. Tissue is modeled as a medium with continuous refractive index (RI) fluctuation and such a fluctuation is described by the RI correlation functions. By measuring optical quantities of tissue (including the scattering power of the OCT spectrum, the reflection albedo α defined as the ratio of scattering coefficient μs, and the backscattering coefficient μb), the RI correlation function can be inversely deduced and the full set of optical scattering properties can be obtained.

    BIOLOGICAL TISSUE ANALYSIS BY INVERSE SPECTROSCOPIC OPTICAL COHERENCE TOMOGRAPHY
    2.
    发明申请
    BIOLOGICAL TISSUE ANALYSIS BY INVERSE SPECTROSCOPIC OPTICAL COHERENCE TOMOGRAPHY 有权
    通过反射光谱光学相干测量的生物组织分析

    公开(公告)号:US20130095519A1

    公开(公告)日:2013-04-18

    申请号:US13651196

    申请日:2012-10-12

    Inventor: Vadim Backman Ji Yi

    CPC classification number: G01N21/4795 A61B5/0066

    Abstract: A method and system to measure and image the full optical scattering properties by inverse spectroscopic optical coherence tomography (ISOCT) is disclosed. Tissue is modeled as a medium with continuous refractive index (RI) fluctuation and such a fluctuation is described by the RI correlation functions. By measuring optical quantities of tissue (including the scattering power of the OCT spectrum, the reflection albedo α defined as the ratio of scattering coefficient μs, and the back-scattering coefficient μb), the RI correlation function can be inversely deduced and the full set of optical scattering properties can be obtained.

    Abstract translation: 公开了通过逆光谱光学相干断层扫描(ISOCT)测量和成像全部光散射特性的方法和系统。 组织被建模为具有连续折射率(RI)波动的介质,并且这种波动由RI相关函数描述。 通过测量组织的光学量(包括OCT光谱的散射功率,被定义为散射系数μ的比率的反射反照率α和背散射系数mub),RI相关函数可以被逆推并且全集 的光散射特性。

    Methods and apparatus for laser scanning structured illumination microscopy and tomography
    7.
    发明授权
    Methods and apparatus for laser scanning structured illumination microscopy and tomography 有权
    激光扫描结构光学显微镜和断层扫描的方法和装置

    公开(公告)号:US09360660B2

    公开(公告)日:2016-06-07

    申请号:US13902288

    申请日:2013-05-24

    Abstract: Certain examples provide a structured illumination microscopy system. The example system includes a laser source to generate excitation illumination directed toward a target. The example system includes a modulator to modulate the excitation illumination temporally in a controllable spatial pattern to be constructed on the target object to provide sub-diffractional resolution in a lateral direction with respect to the target. The example system includes two synchronized laser scanning mirror units in confocal arrangement, the laser scanning units to be synchronized and controlled by a computing device, a first of the scanning mirror units to receive the modulated excitation illumination and project the modulated excitation illumination on the target object and a second of the scanning mirror units to receive emission fluorescence from the target and project the emission fluorescence. The example system includes a detector to collect emission fluorescence from the target via the second of the scanning mirror units.

    Abstract translation: 某些实例提供了结构化的照明显微镜系统。 该示例系统包括产生朝向目标的激发照明的激光源。 该示例系统包括一个调制器,用于以可控的空间图案临时调制激励照明,以在目标物体上构造,以在相对于目标的横向方向上提供子衍射分辨率。 示例系统包括共焦排列的两个同步的激光扫描镜单元,由计算装置同步和控制的激光扫描单元,用于接收经调制的激发照明并将调制的激发照明投影到目标上的第一扫描镜单元 物体和第二个扫描镜单元,以从目标接收发射荧光并投射发射荧光。 该示例系统包括用于经由第二扫描反射镜单元从目标物体收集发射荧光的检测器。

    METHODS AND APPARATUS FOR LASER SCANNING STRUCTURED ILLUMINATION MICROSCOPY AND TOMOGRAPHY
    8.
    发明申请
    METHODS AND APPARATUS FOR LASER SCANNING STRUCTURED ILLUMINATION MICROSCOPY AND TOMOGRAPHY 有权
    激光扫描结构照明显微镜和TOMOGRAPHY的方法和装置

    公开(公告)号:US20130314717A1

    公开(公告)日:2013-11-28

    申请号:US13902288

    申请日:2013-05-24

    Abstract: Certain examples provide a structured illumination microscopy system. The example system includes a laser source to generate excitation illumination directed toward a target. The example system includes a modulator to modulate the excitation illumination temporally in a controllable spatial pattern to be constructed on the target object to provide sub-diffractional resolution in a lateral direction with respect to the target. The example system includes two synchronized laser scanning mirror units in confocal arrangement, the laser scanning units to be synchronized and controlled by a computing device, a first of the scanning mirror units to receive the modulated excitation illumination and project the modulated excitation illumination on the target object and a second of the scanning mirror units to receive emission fluorescence from the target and project the emission fluorescence. The example system includes a detector to collect emission fluorescence from the target via the second of the scanning mirror units.

    Abstract translation: 某些实例提供了结构化的照明显微镜系统。 该示例系统包括产生朝向目标的激发照明的激光源。 该示例系统包括一个调制器,用于以可控的空间图案临时调制激励照明,以在目标物体上构造,以在相对于目标的横向方向上提供子衍射分辨率。 示例系统包括共焦排列的两个同步的激光扫描镜单元,由计算装置同步和控制的激光扫描单元,用于接收经调制的激发照明并将调制的激发照明投影到目标上的第一扫描镜单元 物体和第二个扫描镜单元,以从目标接收发射荧光并投射发射荧光。 该示例系统包括用于经由第二扫描反射镜单元从目标物体收集发射荧光的检测器。

    Biological tissue analysis by inverse spectroscopic optical coherence tomography

    公开(公告)号:US10241041B2

    公开(公告)日:2019-03-26

    申请号:US15590745

    申请日:2017-05-09

    Inventor: Vadim Backman Ji Yi

    Abstract: A method and system to measure and image the full optical scattering properties by inverse spectroscopic optical coherence tomography (ISOCT) is disclosed. Tissue is modeled as a medium with continuous refractive index (RI) fluctuation and such a fluctuation is described by the RI correlation functions. By measuring optical quantities of tissue (including the scattering power of the OCT spectrum, the reflection albedo α defined as the ratio or scattering coefficient μs, and the back-scattering coefficient μb), the RI correlation function can be inversely deduced and the full set of optical scattering properties can be obtained.

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