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    • 3. 发明授权
    • Method for reconstructing a fluorescent image of the interior of a turbid medium and device for imaging the interior of a turbid medium
    • 用于重建浑浊介质内部的荧光图像的方法和用于对浑浊介质的内部进行成像的装置
    • US08520921B2
    • 2013-08-27
    • US12933887
    • 2009-03-20
    • Ronny ZieglerAndy ZieglerTim Nielsen
    • Ronny ZieglerAndy ZieglerTim Nielsen
    • G06K9/00
    • A61B5/4312A61B5/0091G01N21/4795G01N21/6428
    • A method for reconstructing a fluorescence image of the interior of a turbid medium is provided. The method comprises the step: accommodating a turbid medium (1) to which a fluorescent contrast agent has been administered in a measurement volume (4). The fluorescent contrast agent is capable of emitting light in a first range of wavelengths upon irradiation with light. The method further comprises: performing attenuation measurements at a plurality of different wavelengths (λi, . . . , λk) by subsequently irradiating the turbid medium (1) with light from a plurality of different source positions and detecting light emanating from the turbid medium (1) in a plurality of detection positions for each source position; reconstructing absorption properties (μa(r, λ) as a function of the position in the interior of the turbid medium (1) for the plurality of different wavelengths from the attenuation measurements; calculating absorption properties as a function of the position in the interior of the turbid medium (1) for wavelengths of the first range of wavelengths; performing a fluorescence measurement by subsequently irradiating the turbid medium (1) with light causing the fluorescent contrast agent to emit light in the first range of wavelengths from the plurality of source positions and detecting the light emanating from the fluorescent contrast agent in the plurality of detection positions for each source position; and reconstructing a fluorescence image of the spatial distribution of the fluorescent contrast agent in the interior of the turbid medium (1) from the fluorescence measurement using the calculated absorption properties.
    • 提供了一种用于重建浑浊介质内部的荧光图像的方法。 该方法包括以下步骤:在测量体积(4)中容纳已投与荧光造影剂的混浊介质(1)。 荧光造影剂能够在照射光时在第一波长范围内发光。 该方法还包括:通过随后用来自多个不同源位置的光照射浑浊介质(1)并检测从浑浊介质发出的光,以多个不同波长(兰德,兰布克)进行衰减测量 1)在每个源位置的多个检测位置; 根据衰减测量重建吸收性质(mu(r,λ))作为多个不同波长的混浊介质(1)内部的位置的函数;计算作为内部位置的函数的吸收特性 用于波长第一波长范围的混浊介质(1);通过随后用引起荧光对比剂的光在多个源位置发射第一波长范围内的光来照射浑浊介质来进行荧光测量 以及在每个源位置的多个检测位置中检测从荧光对比剂发出的光;以及从所述荧光测量中使用所述荧光测量重建所述浑浊介质(1)内的荧光对比剂的空间分布的荧光图像,使用 计算吸收性能。
    • 4. 发明申请
    • METHOD FOR RECONSTRUCTING A FLUORESCENT IMAGE OF THE INTERIOR OF A TURBID MEDIUM AND DEVICE FOR IMAGING THE INTERIOR OF A TURBID MEDIUM
    • 用于重建涡轮介质内部的荧光图像的方法和用于成像涡轮介质的内部的装置
    • US20110026851A1
    • 2011-02-03
    • US12933887
    • 2009-03-20
    • Ronny ZieglerAndy ZieglerTim Nielsen
    • Ronny ZieglerAndy ZieglerTim Nielsen
    • G06K9/40G01J1/58
    • A61B5/4312A61B5/0091G01N21/4795G01N21/6428
    • A method for reconstructing a fluorescence image of the interior of a turbid medium is provided. The method comprises the step: accommodating a turbid medium (1) to which a fluorescent contrast agent has been administered in a measurement volume (4). The fluorescent contrast agent is capable of emitting light in a first range of wavelengths upon irradiation with light. The method further comprises: performing attenuation measurements at a plurality of different wavelengths (λi, . . . λk) by subsequently irradiating the turbid medium (1) with light from a plurality of different source positions and detecting light emanating from the turbid medium (1) in a plurality of detection positions for each source position; reconstructing absorption properties (μa(r, λ)) as a function of the position in the interior of the turbid medium (1) for the plurality of different wavelengths from the attenuation measurements; calculating absorption properties as a function of the position in the interior of the turbid medium (1) for wavelengths of the first range of wavelengths; performing a fluorescence measurement by subsequently irradiating the turbid medium (1) with light causing the fluorescent contrast agent to emit light in the first range of wavelengths from the plurality of source positions and detecting the light emanating from the fluorescent contrast agent in the plurality of detection positions for each source position; and reconstructing a fluorescence image of the spatial distribution of the fluorescent contrast agent in the interior of the turbid medium (1) from the fluorescence measurement using the calculated absorption properties.
    • 提供了一种用于重建浑浊介质内部的荧光图像的方法。 该方法包括以下步骤:在测量体积(4)中容纳已投与荧光造影剂的混浊介质(1)。 荧光造影剂能够在照射光时在第一波长范围内发光。 该方法还包括:通过随后用来自多个不同源位置的光照射混浊介质(1)并检测从浑浊介质(1)发出的光,在多个不同波长(λ1,...λk)下执行衰减测量 )在每个源位置的多个检测位置中; 根据衰减测量,重建作为多个不同波长的混浊介质(1)内部位置的函数的吸收特性(μa(r,λ)); 计算作为第一波长范围波长的混浊介质(1)内部位置的函数的吸收特性; 通过随后用引起荧光对比剂的光在多个源位置的第一波长范围内发射光,并在多个检测中检测从荧光对比剂发出的光,进行荧光测量 每个来源职位的职位; 以及使用所计算的吸收特性,从所述荧光测量重建所述浑浊介质(1)内的所述荧光造影剂的空间分布的荧光图像。
    • 5. 发明申请
    • IMAGING OF A TURBID MEDIUM
    • 涡轮介质的成像
    • US20100014084A1
    • 2010-01-21
    • US12518891
    • 2007-12-12
    • Ronny ZieglerTim Nielsen
    • Ronny ZieglerTim Nielsen
    • G01N21/84
    • G01N21/4795A61B5/0091A61B5/4312
    • An imaging system for imaging of a turbid medium comprises a radiation source to illuminate an object to be imaged. A detection system detects radiation from the object and includes a separation module which distinguishes radiation components having respective wavelength ranges. An analysis module forms a comparison of respective radiation components. An image dataset is reconstructed on the basis of the comparison of respective radiation components. The comparison e.g. involves (i) the ratio of the levels of the high-wavelength radiation component to the low-wavelength radiation component, or (ii) i the relative difference of the levels of high-wavelength radiation component to the detected radiation, or (iiii) the relative difference of the levels of the high-wavelength radiation component to the low-wavelength radiation component. Good contrast in the reconstructed image is achieved when the comparison is relatively more beneficial to one of the wavelength ranges to the other ones over the relevant range of concentration of contrast agent. Accordingly, in the comparison competition among wavelength ranges is such that the intensity (or photon count) of that one wavelength range dominates so that any contrast in that one wavelength range does not suffer from contrast inversion.
    • 用于对混浊介质进行成像的成像系统包括用于照射待成像物体的辐射源。 检测系统检测来自物体的辐射,并且包括区分具有各个波长范围的辐射分量的分离模块。 分析模块形成各个辐射分量的比较。 基于各个辐射分量的比较来重建图像数据集。 比较例如 涉及(i)高波长辐射分量与低波长辐射分量的比例,或(ii)i是高波长辐射分量与检测到的辐射的相对差,或者(iiii) 高波长辐射分量与低波长辐射分量的相对差异。 当比较在造影剂浓度的相关范围内比较对其中一个波长范围相对更有利时,可以实现重建图像中的良好的对比度。 因此,在波长范围内的比较比较中,使得该一个波长范围的强度(或光子计数)成为主导,使得该一个波长范围内的任何对比度都不会遭受对比反转。
    • 6. 发明授权
    • Imaging of a turbid medium
    • 浑浊介质成像
    • US07986411B2
    • 2011-07-26
    • US12518891
    • 2007-12-12
    • Ronny ZieglerTim Nielsen
    • Ronny ZieglerTim Nielsen
    • G01N21/00
    • G01N21/4795A61B5/0091A61B5/4312
    • An imaging system for imaging of a turbid medium comprises a radiation source to illuminate an object to be imaged. A detection system detects radiation from the object and includes a separation module which separates and distinguishes radiation components having respective wavelength ranges. An analysis module forms a comparison of respective radiation components. An image dataset is reconstructed on the basis of the comparison of respective radiation components. The comparison may involve the ratio of the levels of the high-wavelength radiation component to the low-wavelength radiation component, the relative difference of the levels of high-wavelength radiation component to the detected radiation, and the relative difference of the levels of the high-wavelength radiation component to the low-wavelength radiation component.
    • 用于对混浊介质进行成像的成像系统包括用于照射待成像物体的辐射源。 检测系统检测来自物体的辐射,并且包括分离和区分具有各个波长范围的辐射分量的分离模块。 分析模块形成各个辐射分量的比较。 基于各个辐射分量的比较来重建图像数据集。 该比较可以包括高波长辐射分量与低波长辐射分量的比值,高波长辐射分量的水平与检测到的辐射的相对差异,以及 高波长辐射分量到低波长辐射分量。
    • 10. 发明申请
    • Iterative Image Reconstruction of a Moving Object From Projection Data
    • 投影数据中移动物体的迭代图像重建
    • US20080267480A1
    • 2008-10-30
    • US12097544
    • 2006-12-08
    • Tim NielsenMichael GrassAndy Ziegler
    • Tim NielsenMichael GrassAndy Ziegler
    • G06T11/00
    • G06T11/006G06T2211/412G06T2211/424
    • Iterative methods for reconstructing an image sequence of a moving object based on projection data usually require a high computationally effort. According to embodiments of the present invention there is provided such a method wherein a first image representing the object at a first phase is used as an initial image for iteratively reconstructing a second image at a second phase. A first gating function is assigned to the first phase, a second gating function is assigned to the second phase. When executing a first iteration for reconstructing the second image only projection data corresponding to a non-overlapping part of the two gating functions are used. For executing further iterations the amount of projection data corresponding to the overlapping part of the two gating functions may be gradually increased. Therefore, for all further but the last iteration the computationally effort is significantly reduced. However, this low computationally expense has no negative impact on the quality of the finally reconstructed second image because the method benefits from the fact that the first image was used as the initial image for iteratively reconstructing the second image.
    • 基于投影数据重建移动物体的图像序列的迭代方法通常需要较高的计算量。 根据本发明的实施例,提供了这样的方法,其中将表示第一阶段的对象的第一图像用作用于在第二阶段迭代重建第二图像的初始图像。 第一门控功能被分配给第一阶段,第二门控功能被分配给第二阶段。 当执行用于重构第二图像的第一次迭代时,仅使用与两个门控功能的非重叠部分相对应的投影数据。 为了执行进一步的迭代,可以逐渐增加对应于两个门控功能的重叠部分的投影数据量。 因此,对于所有进一步但最后的迭代,计算量的努力显着降低。 然而,这种低的计算费用对最终重建的第二图像的质量没有负面影响,因为该方法受益于第一图像被用作用于迭代重建第二图像的初始图像的事实。