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    • 3. 发明授权
    • NMR imaging method
    • NMR成像方法
    • US4853636A
    • 1989-08-01
    • US141788
    • 1988-01-11
    • Etsuji YamamotoYukiko OguraHideki Kohno
    • Etsuji YamamotoYukiko OguraHideki Kohno
    • G01R33/54
    • G01R33/4833
    • An NMR imaging method for obtaining a tomographic image of an object through two-dimensional Fourier transformation imaging. After a whole image of a predetermined slice is displayed, a given field of view having a given size and located at a given position in the image is designated. On the basis of data derived from this designation, setting values for magnetic field generators and a signal detector are arithmetically determined for limiting the region in which the NMR signal is generated and the region to be imaged, whereby local imaging of the aforementioned field of view is conducted with high resolution. Further, division of an image resulting from the imaging operation is automatically corrected by exchanging positionally the divided image blocks with each other.
    • 一种用于通过二维傅里叶变换成像获得物体的断层图像的NMR成像方法。 在显示预定切片的整个图像之后,指定具有给定尺寸并且位于图像中的给定位置的给定视场。 基于从该指定导出的数据,算术地确定用于限制产生NMR信号的区域和要成像的区域的磁场发生器和信号检测器的设定值,由此上述视野的局部成像 以高分辨率进行。 此外,通过将分割的图像块彼此交换而自动地校正由成像操作产生的图像的划分。
    • 4. 发明授权
    • Method and system for determining electromotive force or impressed
current distribution in an object based on magnetic field distribution
measured outside the object
    • 基于在物体外部测量的磁场分布来确定物体中的电动势或外加电流分布的方法和系统
    • US5426365A
    • 1995-06-20
    • US13425
    • 1993-02-04
    • Kensuke SekiharaYukiko Ogura
    • Kensuke SekiharaYukiko Ogura
    • A61B5/05A61B5/04A61B5/053G01R33/00G01R33/02G01R33/035G01R33/10
    • G01R33/02A61B5/04008A61B5/0536
    • In a magnetic field generation source measuring method and system for determining a magnetic field generation source in an object to be examined from a magnetic field in the interior of the object measured at the exterior of the object, the object is represented by a model in which the object is divided into a plurality of cells. The resistance values of each cell in x, y and z directions are determined from information concerning the electric conductivity of the interior of the object beforehand measured. Supposing the distribution of electromotive forces in the object as a current source, a return current generated in accordance with the electromotive force distribution in the object is determined by use of estimated values of the intensities of the current source in the x, y and z directions and the resistance values. A vector of the sum of a current of the current source and the return current is determined for all of the cells. The second power of the absolute value of a difference between the vector of the sum and a current vector determined from the magnetic field in the interior of the object measured at the exterior of the object is subjected to summation for all of the cells. The estimated values of the current source intensities, which minimize the summation, are determined as an electromotive force distribution in the object.
    • 在用于在物体外部测量的物体内部的磁场中确定待检测物体中的磁场产生源的磁场产生源测量方法和系统中,该对象由以下模型表示:其中, 该对象被分成多个单元。 x,y和z方向上的每个单元的电阻值由预先测量的物体内部的电导率的信息确定。 假设物体中的电动势作为电流源的分布,通过使用x,y和z方向上的电流源的强度的估计值来确定根据物体中的电动势分布产生的返回电流 和电阻值。 为所有单元确定电流源的电流和返回电流之和的向量。 在对象外部测量的对象内部的磁场确定的和矢量的矢量和当前矢量之间的差的绝对值的第二功率对所有单元进行求和。 将求和的最小值的电流源强度的估计值确定为物体中的电动势分布。