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    • 1. 发明授权
    • NMR imaging method
    • NMR成像方法
    • US4739265A
    • 1988-04-19
    • US846151
    • 1986-03-31
    • Etsuji YamamotoKensuke SekiharaHidemi ShionoHideki Kohno
    • Etsuji YamamotoKensuke SekiharaHidemi ShionoHideki Kohno
    • G01R33/485G01R33/565G01R33/20
    • G01R33/565G01R33/485G01R33/56527
    • A method for providing spin density distribution images of an object, discriminated with respect to plural chemical shifts. This method is performed by repeating a measurement sequence in a spin warp imaging method, of the spin data plural times, with a time difference .DELTA..tau. between a time interval .tau..sub.1 from spin excitation to a 180.degree. RF pulse and a time interval .tau..sub.2 from the 180.degree. RF pulse to a peak of a spin echo, altering .DELTA..tau. in the ways corresponding the number of chemical shifts to be discriminated from one another, subjecting the respective spin data to two-dimensional Fourier transform to provide plural sets of spin data for respective coordinates in a spatial domain, and solving simultaneous equations of the sets of spin data to provide spin densities corresponding to the respective chemical shifts.
    • 一种用于提供对象的自旋密度分布图像的方法,其被鉴别为多个化学位移。 该方法通过在旋转数据成像方法中重复自旋数据多次的测量序列,其中从自旋激发到180°RF脉冲的时间间隔τ1与时间间隔τ2之间的时间差DELTAτ 从180°RF脉冲到自旋回波的峰值,以相应于要彼此区分的化学位移数的方式改变DELTA tau,对各自旋转数据进行二维傅里叶变换以提供多组旋转 用于空间域中的各个坐标的数据,以及求解自旋数据组的联立方程以提供对应于各个化学位移的自旋密度。
    • 2. 发明授权
    • High speed imaging method with three-dimensional NMR
    • 高速成像方法采用三维NMR
    • US4716369A
    • 1987-12-29
    • US746663
    • 1985-06-20
    • Kensuke SekiharaShigeru MatsuiHideki KohnoEtsuji YamamotoHidemi Shiono
    • Kensuke SekiharaShigeru MatsuiHideki KohnoEtsuji YamamotoHidemi Shiono
    • G01R33/485G01R33/561G01R33/20
    • G01R33/485G01R33/5615G01R33/5616
    • The present invention is an imaging method using three-dimensional NMR to which an echo-planar method is applied. After excitation of nuclear spins, the gradient magnetic field Gx for phase-encoding is applied and there is repeated a sequence of measuring and obtaining an echo train of spin-echoes with a constant gradient magnetic field Gx and a periodically-inverted gradient magnetic field Gy, as varying the amount of encoding, so as to obtain the three-dimensional imaging by the Fourier-conversion. Moreover, after the selective excitation of spins within an X-Y surface, a 180.degree. radio frequency pulse is applied. As varying the time difference .tau..sub..epsilon. between the interval from the excitation until the application of the 180.degree. radio frequency pulse and the interval from the application thereof until a peak of a first echo of an echo train, three-dimensional imaging is carried out with a chemical shift axis as one axis by repeating the sequence and accomplishing Fourier-conversion with .tau..sub..epsilon. as a numerical variable.
    • 本发明是使用采用回波平面法的三维NMR的成像方法。 在激励核自旋之后,施加用于相位编码的梯度磁场Gx,并且重复测量并获得具有恒定梯度磁场Gx和周期性反转梯度磁场Gy的自旋回波回波序列的序列 ,因为改变编码量,从而通过傅里叶变换获得三维成像。 此外,在X-Y表面中的自旋选择性激发之后,施加180°射频脉冲。 随着从激励到施加180°射频脉冲的间隔与从应用到应用的间隔直到回波列的第一回波的峰值之间的时间差τεε改变,三维成像是 化学位移轴作为一个轴,通过重复该序列,并以tauε作为数值变量进行傅里叶变换。
    • 6. 发明授权
    • Method of measuring the static magnetic field distribution in an NMR
inspection system
    • 在NMR检查系统中测量静态磁场分布的方法
    • US4672318A
    • 1987-06-09
    • US696909
    • 1985-01-31
    • Kensuke SekiharaEtsuji YamamotoShigeru MatsuiHideki Kohno
    • Kensuke SekiharaEtsuji YamamotoShigeru MatsuiHideki Kohno
    • G01R33/20A61B5/055A61B10/00G01R33/24G01R33/38G01R33/387
    • G01R33/24
    • A method of measuring a static magnetic field distribution in a nuclear magnetic resonance (NMR) inspection system which comprises magnetic field generator for producing a static magnetic field, inclination or gradient magnetic fields and a high-frequency magnetic field, a signal detector for sensing nuclear magnetic resonance signals from an inspection sample, a computer for processing output signals from the signal detector and an output device for providing a computational result of the computer, wherein a time interval t.sub.1 from the center of a 90.degree.-pulse high-frequency magnetic field to the center of a 180.degree.-pulse high-frequency magnetic field is made different by a time difference t.sub.0 from a time interval t.sub.2 from the center of the 180.degree.-pulse high-frequency magnetic field to a peak of a spin echo, so that static magnetic field distribution is calculated based on the computer output which corresponds to the difference of the two time intervals.
    • 一种在核磁共振(NMR)检查系统中测量静磁场分布的方法,其包括用于产生静磁场,倾斜或梯度磁场和高频磁场的磁场发生器,用于感测核的信号检测器 来自检查样本的磁共振信号,用于处理来自信号检测器的输出信号的计算机和用于提供计算机的计算结果的输出装置,其中从90°脉冲高频磁场的中心起的时间间隔t1 从180°脉冲高频磁场的中心到从180°脉冲高频磁场的中心到自旋回波的峰值的时间间隔t2由时间差t0变化到180°脉冲高频磁场的中心,因此 基于对应于两个时间间隔的差的计算机输出来计算静态磁场分布。
    • 8. 发明授权
    • NMR imaging method
    • NMR成像方法
    • US4760339A
    • 1988-07-26
    • US944001
    • 1986-12-22
    • Etsuji YamamotoKoichi SanoHidemi ShionoHideki Kohno
    • Etsuji YamamotoKoichi SanoHidemi ShionoHideki Kohno
    • A61B10/00A61B5/055G01R33/48G01R33/485G01R33/565G01R33/20
    • G01R33/565G01R33/485G01R33/56527
    • An NMR imaging method is disclosed in which an object is measured in accordance with a pulse sequence capable of expressing a difference between two of a plurality of chemical shifts by a phase difference in a signal, that is, a pulse sequence 90.degree.-.tau..sub.a -180.degree.-.tau..sub.b -spin echo (where .tau..sub.a .noteq..tau..sub.b) to obtain spin distribution data, a histogram with respect to the phase of the spin distribution data is formed to regard a phase corresponding to that one of a plurality of peaks of the histogram which exists at one end of the histogram, as a position-independent offset phase which is contained in the spin distribution data and is peculiar to an NMR imaging apparatus, and the spin distribution data is corrected using the offset value thus obtained, to extract spin density distribution data for each of the chemical shifts from the corrected spin distribution data.
    • 公开了一种NMR成像方法,其中根据能够通过信号的相位差表示多个化学位移之间的差异的脉冲序列来测量物体,即脉冲序列90°-τa -180°-τb-自旋回波(其中τa NOTEQUAL tau b)为了获得自旋分布数据,形成相对于自旋分布数据的相位的直方图,以考虑与多个峰中的那一个相对应的相位 存在于直方图的一端的直方图作为自旋分布数据中包含的并且是NMR成像设备特有的与位置无关的偏移相位,并且使用由此获得的偏移值来校正自旋分布数据, 从校正的自旋分布数据中提取每个化学位移的自旋密度分布数据。
    • 10. 发明授权
    • Nuclear magentic resonance imaging apparatus
    • 核磁共振成像装置
    • US5465719A
    • 1995-11-14
    • US98775
    • 1993-07-29
    • Hiroyuki ItagakiYo TaniguchiHidemi ShionoKenji TakiguchiEtsuji Yamamoto
    • Hiroyuki ItagakiYo TaniguchiHidemi ShionoKenji TakiguchiEtsuji Yamamoto
    • A61B5/055G01R33/20G01R33/28G01R33/38G01R33/385H01F7/20
    • G01R33/385G01R33/3802G01R33/3854
    • A bobbin for holding a gradient magnetic field coil, having a changeable size and sectional shape (a separable bobbin) is constituted by assembling coil supporters (a bobbin divided into a plurality of segments). The separable bobbin has coil supporters of an upper part a bottom part and a set of side surface parts and at least two supporting rods made of a nonmagnetic substance are fitted to the side surface parts of the coil supporters. Holes permitting the insertion of the supporting rods are bored in the upper and bottom parts of the coil supporters. The length d1 between both side surface parts can be made variable by adjusting the insertion length of the supporting rod into the upper and bottom parts. Accordingly, the distance between a patient and a gradient magnetic field can be reduced, and an intended gradient magnetic field intensity can be generated by a smaller current producing the gradient magnetic field than in the prior art. Setting of the patient to an MRI imaging apparatus becomes also easier, and there can be obtained a gradient magnetic field coil capable of being easily fitted and removed to and from the MRI imaging apparatus.
    • 用于保持具有可变尺寸和截面形状(分离线圈架)的梯度磁场线圈的线轴由线圈支架(分为多个段的线轴)组装而成。 可分离筒管具有上部的线圈支撑件,底部部分和一组侧面部分,并且至少两个由非磁性物质制成的支撑杆装配到线圈支撑件的侧表面部分。 允许插入支撑杆的孔在线圈支撑件的上部和底部中钻孔。 通过将支撑杆的插入长度调节到上部和底部,两个侧面部分之间的长度d1可以变化。 因此,可以减少患者与梯度磁场之间的距离,并且通过产生梯度磁场的较小电流可以产生预期的梯度磁场强度,而不是现有技术。 将患者设置到MRI成像设备变得更容易,并且可以获得能够容易地装配和去除MRI成像设备的梯度磁场线圈。