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    • 11. 发明授权
    • Split type magnetic field generating apparatus for MRI
    • 用于MRI的分割型磁场产生装置
    • US5939962A
    • 1999-08-17
    • US906001
    • 1997-08-04
    • Yasuyuki TaharaHajime TanabeHirotaka Takeshima
    • Yasuyuki TaharaHajime TanabeHirotaka Takeshima
    • G01R33/38G01R33/381H01F5/08
    • G01R33/381G01R33/3806
    • Annular portions are arranged on mutually confronting surfaces at circumferential edge portions of low-temperature containers, the annular portions forming annular containing portions whose cross section is rectangular. Not only a side coil among a group of coils forming a collective coil body is disposed inside the containing portion, but also a gradient magnetic field unit, a radio-frequency transmission coil, and a reception coil are disposed inside a recessed portion so as to be integrated with one another into a single body, the recessed portion being formed so as to be surrounded by the corresponding annular portion. The side coil supplies more than half a designed magnetomotive force. Since a distance J of the mutually confronting low-temperature containers, i.e., the distance between the mutually confronting surfaces of the side coils can be reduced by a distance corresponding to the projection of the projected portions, not only the designed magnetomotive force can be reduced, but also the apparatus can be downsized and inexpensive.
    • 环状部分布置在低温容器的圆周边缘部分的相互面对的表面上,环形部分形成截面为矩形的环形容纳部分。 形成集体线圈体的一组线圈中的侧线圈不仅设置在容纳部内,而且还设置有倾斜磁场单元,射频发送线圈和接收线圈, 彼此一体地形成为一体,该凹部被形成为被相应的环形部分包围。 侧线圈提供超过一半设计的磁动力。 由于相互面对的低温容器的距离J,即侧面线圈的相互面对的面之间的距离可以减小与突出部分的突起相对应的距离,不仅可以减小设计的磁动势 ,而且该装置也可以小型化和便宜化。
    • 12. 发明授权
    • Magnetic resonance imaging apparatus
    • 磁共振成像装置
    • US07605587B2
    • 2009-10-20
    • US11791878
    • 2005-11-29
    • Hirotaka Takeshima
    • Hirotaka Takeshima
    • G01V3/00
    • A61B5/055G01R33/3806G01R33/381G01R33/3815G01R33/385G01R33/4215G01R33/422
    • A magnetic resonance imaging apparatus is provide that includes static magnetic field generation means arranged around an imaging space where an examinee is to be located and generating a static magnetic field in the imaging space; gradient magnetic field generation means arranged in the imaging space side of the static magnetic field generation means and generating a gradient magnetic field in the imaging space; and high-frequency magnetic field generation means arranged at the imaging space side of the gradient magnetic field generation means and generating a high-frequency magnetic field in the imaging space. The gradient magnetic field generation means has a concave portion in the vicinity of the imaging space depressed toward the static magnetic field generation means. At least a part of the high-frequency magnetic field generation means is contained in the concave portion.
    • 提供一种磁共振成像装置,其包括围绕成像空间布置的静态磁场产生装置,其中被检体将被定位并在成像空间中产生静态磁场; 设置在静磁场产生装置的成像空间侧的梯度磁场产生装置,并在成像空间中产生梯度磁场; 以及高频磁场产生装置,其布置在所述倾斜磁场产生装置的成像空间侧并在所述成像空间中产生高频磁场。 梯度磁场产生装置在静止磁场产生装置上朝向成像空间附近具有凹部。 高频磁场产生装置的至少一部分包含在凹部中。
    • 16. 发明授权
    • Method of calculating coil pattern, and gradient magnetic field coil
    • 线圈图案计算方法和梯度磁场线圈
    • US08581586B2
    • 2013-11-12
    • US12933255
    • 2009-03-27
    • Mitsushi AbeHirotaka Takeshima
    • Mitsushi AbeHirotaka Takeshima
    • G01V3/00
    • G01R33/385
    • A coil pattern calculation method includes calculating a current potential at each contact between finite surface elements forming each of the coil surfaces based on an initial value of an input current potential distribution, and, for each of the coil surfaces, repeatedly calculating the current potential alternately and, under each magnetic field condition, determining a current potential distribution that generates a magnetic field falling within the range of allowable error for each target magnetic field so that a surface current represented by the current potential will become close to a target magnetic field distribution set for each of the finite surface elements; and determining a coil pattern from the contour lines of the determined current potential distribution.
    • 线圈图案计算方法包括基于输入电流分布的初始值来计算形成每个线圈表面的有限表面元件之间的每个接触处的电流电位,并且对于每个线圈表面,交替重复地计算电流电势 并且在每个磁场条件下,确定产生每个目标磁场的容许误差范围内的磁场的电流分布,使得由电流电位表示的表面电流将变得接近目标磁场分布集 对于每个有限表面元素; 以及从所确定的电流分布的轮廓线确定线圈图案。
    • 17. 发明申请
    • METHOD OF CALCULATING COIL PATTERN, AND GRADIENT MAGNETIC FIELD COIL.
    • 计算线圈图案和梯度磁场线圈的方法。
    • US20110018540A1
    • 2011-01-27
    • US12933255
    • 2009-03-27
    • Mitsushi AbeHirotaka Takeshima
    • Mitsushi AbeHirotaka Takeshima
    • G01R33/44
    • G01R33/385
    • The present invention eliminate the limitation of coil pattern design, facilitates the fabrication, and improves the accuracy of magnetic field. A coil pattern calculation method is characterized by comprising the steps of: calculating a current potential at each contact between finite surface elements forming each of the coil surfaces based on an initial value of an input current potential distribution, and, for each of the coil surfaces, repeatedly calculating the current potential alternately and, under each magnetic field condition, determining a current potential distribution that generates a magnetic field falling within the range of allowable error for each target magnetic field so that a surface current represented by the current potential will become close to a target magnetic field distribution set for each of the finite surface elements; and determining a coil pattern from the contour lines of the determined current potential distribution.
    • 本发明消除了线圈图案设计的限制,便于制造,并且提高了磁场的精度。 线圈图案计算方法的特征在于包括以下步骤:基于输入电流分布的初始值来计算形成每个线圈表面的有限表面元件之间的每个接触处的电流电势,并且对于每个线圈表面 ,交替地重复计算电流,并且在每个磁场条件下,确定产生每个目标磁场的容许误差范围内的磁场的电流分布,使得由当前电位表示的表面电流变得接近 到每个有限表面元件的目标磁场分布集合; 以及从所确定的电流分布的轮廓线确定线圈图案。
    • 18. 发明授权
    • Magnetic resonance imaging system
    • 磁共振成像系统
    • US06876198B2
    • 2005-04-05
    • US10380115
    • 2001-09-11
    • Shigeru WatanabeTetsuhiko TakahashiHirotaka TakeshimaHiromichi Shimizu
    • Shigeru WatanabeTetsuhiko TakahashiHirotaka TakeshimaHiromichi Shimizu
    • A61B5/055G01R33/28G01R33/54G01R33/561G01V3/00
    • G01R33/285A61B5/055G01R33/54G01R33/5611
    • A magnetic resonance imaging apparatus is provided with a sequencer for executing a rapid imaging sequence of up to 100 ms at a full scan, a parallel measurement system for executing a partial encoding measurement in which the number of phase encoding operations performed for the measurement is reduced, an image processing system for reconstructing images from the information obtained though parallel measurements and composing reconstructed images of a plurality of areas to make one image, a display system for displaying the obtained images at a rate of 50 frame/second or more, and an image renewal system for taking in coordinate information of the cross-section to be imaged from position and pointing devices at intervals of about 0.1 second, and renewing the cross-section to be imaged in real time. Thus, imaging on the cross-sections indicated by a device can be performed in real time with high spatial and high time resolution.
    • 磁共振成像装置设置有用于在全扫描时执行高达100ms的快速成像序列的定序器,用于执行部分编码测量的并行测量系统,其中对测量执行的相位编码操作的数量减少 ,图像处理系统,用于根据通过并行测量获得的信息重构图像,并且构成多个区域的重建图像以形成一个图像;显示系统,用于以50帧/秒以上的速率显示所获得的图像;以及 图像更新系统,用于以约0.1秒的间隔获取要从位置和指点设备成像的横截面的坐标信息,并实时更新要成像的横截面。 因此,可以以高空间和高时间分辨率实时地执行由装置指示的横截面上的成像。
    • 19. 发明授权
    • Magnetic resonance imaging apparatus
    • 磁共振成像装置
    • US06498488B2
    • 2002-12-24
    • US09992356
    • 2001-11-13
    • Hirotaka TakeshimaYoshihide Wadayama
    • Hirotaka TakeshimaYoshihide Wadayama
    • G01V300
    • G01R33/383G01R33/56518
    • A magnetic resonance imaging apparatus is provided with a pair of static magnetic field uniformity controlling members 30A and 30B which are disposed adjacent to respective pair of magnetic plates 25A and 25B and of which cross sections configured so as to further enhance static magnetic field uniformity in static magnetic field region 21 and a pair of flat plate shaped eddy current suppressing members 29A and 29B which are disposed adjacent to respective pair of gradient magnetic field coils 28A and 28B and shield influences of gradient magnetic field generated by the gradient magnetic field coils 28A and 28B on the static magnetic field uniformity controlling members 30A and 30B of pole pieces. The eddy current suppressing members 29A and 29B are easily manufactured from a flat plate member simply by cutting the same while following the shape of the gradient magnetic field coils 28A and 28B. Further, with the provision of the eddy current suppressing members 29A and 29B influences due to eddy current and residual magnetism induced by the gradient magnetic field coils 28A and 28B on the static magnetic field uniformity controlling members 30A and 30B are suppressed and uniformity in the uniform static magnetic field region is enhanced.
    • 磁共振成像装置设置有一对静磁场均匀性控制部件30A和30B,这些静止磁场均匀性控制部件30A和30B设置在相应的一对磁性板25A和25B附近,并且其横截面被配置为进一步增强静态磁场均匀性 磁场区域21和与各对梯度磁场线圈28A,28B相邻配置的一对平板状的涡流抑制部件29A,29B以及由倾斜磁场线圈28A,28B产生的倾斜磁场的屏蔽影响 在极片的静磁场均匀性控制构件30A和30B上。 涡流抑制部件29A,29B容易由平板部件简单地通过沿着倾斜磁场线圈28A,28B的形状切割而制作。 此外,由于涡电流抑制部件29A和29B由涡流引起的影响,由静磁场均匀性控制部件30A和30B上的梯度磁场线圈28A和28B引起的剩余磁体被抑制,均匀的均匀性 静磁场区域增强。