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    • 11. 发明授权
    • Magnetic resonance imaging method and apparatus
    • 磁共振成像方法和装置
    • US07372269B2
    • 2008-05-13
    • US10553900
    • 2004-04-23
    • Masahiro TakizawaTetsuhiko TakahashiYo Taniguchi
    • Masahiro TakizawaTetsuhiko TakahashiYo Taniguchi
    • G01V3/00
    • G01R33/4824G01R33/5611
    • In a magnetic resonance imaging apparatus, an RF pulse is applied to a subject placed in a static magnetic field, a plurality of gradient magnetic fields are applied, and induced nuclear magnetic resonance signal (echo signal) is received by means of a RF receiving coil unit composed of two or more RF receiving coils. A parallel MRI method is applied to echo signals acquired by reducing the echoes per blade of a propeller MRI method so as to remove the artifact to produce a reconstructed image. The reconstructed image is subjected to inverse Fourier transform to return it to the echo signals in a measurement space corresponding to the blade. The echo signals are girded in an arbitrarily predetermined coordinate system for image and combined. Such a processing is conducted for the echo signals of all the blades. A final image is reconstructed using the echo signals after the image creation in the coordinate system for image.
    • 在磁共振成像装置中,将RF脉冲施加到放置在静态磁场中的被摄体,施加多个梯度磁场,并且通过RF接收线圈接收感应的核磁共振信号(回波信号) 单元由两个或更多个RF接收线圈组成。 将并行MRI方法应用于通过减小螺旋桨MRI方法的每个叶片的回波而获得的回波信号,以便去除伪影以产生重建图像。 对重构图像进行傅立叶逆变换,将其返回到与叶片对应的测量空间中的回波信号。 回波信号被束缚在用于图像并组合的任意预定的坐标系中。 对所有叶片的回波信号进行这样的处理。 在用于图像的坐标系中的图像创建之后,使用回波信号重建最终图像。
    • 12. 发明申请
    • Magnetic resonance imaging method and apparatus
    • 磁共振成像方法和装置
    • US20060232273A1
    • 2006-10-19
    • US10553900
    • 2004-04-23
    • Masahiro TakizawaTetsuhiko TakahashiYo Taniguchi
    • Masahiro TakizawaTetsuhiko TakahashiYo Taniguchi
    • G01V3/00A61B5/05
    • G01R33/4824G01R33/5611
    • High-speed imaging by a propeller MRI method is enabled as a whole thanks to high-speed computation by preventing an aliasing artifact even if the echoes acquired by one blade are decreased and by reducing the imaging time and the computational complexity. In a magnetic resonance imaging apparatus, an RF pulse is applied to a subject placed in a static magnetic field, a plurality of gradient magnetic fields are applied, and induced nuclear magnetic resonance signal (echo signal) is received by means of a multiple RF receiving coil unit composed of two or more RF receiving coils. A parallel MRI method is applied to echo signals acquired by reducing the echoes per blade of a propeller MRI method so as to remove the artifact to produce a reconstructed image. The reconstructed image is subjected to inverse Fourier transform to return it to the echo signals in a measurement space corresponding to the blade. The echo signals are girded in an arbitrarily predetermined coordinate system for image and combined. Such a processing is conducted for the echo signals of all the blades. A final image is reconstructed using the echo signals after the image creation in the coordinate system for image.
    • 通过螺旋桨MRI方法的高速成像由于高速计算,即使通过防止由一个叶片获得的回波减少并且通过减少成像时间和计算复杂度来防止混叠伪影,也能够实现。 在磁共振成像装置中,将RF脉冲施加到放置在静态磁场中的被摄体,施加多个梯度磁场,并且通过多个RF接收来接收诱导的核磁共振信号(回波信号) 线圈单元由两个或更多个RF接收线圈组成。 将并行MRI方法应用于通过减小螺旋桨MRI方法的每个叶片的回波而获得的回波信号,以便去除伪影以产生重建图像。 对重构图像进行傅立叶逆变换,将其返回到与叶片对应的测量空间中的回波信号。 回波信号被束缚在用于图像并组合的任意预定的坐标系中。 对所有叶片的回波信号进行这样的处理。 在用于图像的坐标系中的图像创建之后,使用回波信号重建最终图像。
    • 14. 发明授权
    • RF probe and inspection system using NMR using the same
    • 射频探头和使用核磁共振的检查系统
    • US5808467A
    • 1998-09-15
    • US653315
    • 1996-05-24
    • Hisaaki OchiYo TaniguchiKenichi OkajimaYoshitaka BitoEtsuji Yamamoto
    • Hisaaki OchiYo TaniguchiKenichi OkajimaYoshitaka BitoEtsuji Yamamoto
    • G01R33/3415G01V3/00
    • G01R33/3415
    • In the inspection system using nuclear magnetic resonance comprising magnetic field generators such as a static magnetic field, a gradient magnetic field, and an RF magnetic field, an RF probe for detecting an NMR signal from a subject, and a calculator for operating a detected signal by the RF probe, a RF probe for detection comprises a plurality of coils arranged in the predetermined direction and includes a plurality of switching elements and the inspection system selects two or more coils from the plurality of coils for each measurement of NMR signals, turns the switching elements connected to the selected coils ON, turns the switching elements connected to coils other than the selected coils OFF, changes a combination of two or more coils for each measurement of NMR signals, and changes the sensitivity distribution of the RF probe in the predetermined direction according to the Wavelet basis function for each measurement of NMR signals.
    • 在使用包括诸如静磁场,梯度磁场和RF磁场的磁场发生器的核磁共振的检查系统中,用于检测来自被检体的NMR信号的RF探针和用于操作检测信号的计算器 通过RF探头,用于检测的RF探针包括沿预定方向布置的多个线圈,并且包括多个开关元件,并且检查系统从每个测量NMR信号中选择来自多个线圈的两个或更多个线圈, 连接到所选择的线圈的开关元件接通,将与所选线圈以外的线圈相连的开关元件断开,对每个NMR信号的测量改变两个或更多个线圈的组合,并将RF探针的灵敏度分布改变为预定的 根据每个NMR信号测量的小波基函数的方向。
    • 15. 发明授权
    • Magnetic resonance imaging apparatus
    • 磁共振成像装置
    • US07868618B2
    • 2011-01-11
    • US12308186
    • 2007-06-12
    • Yo TaniguchiHisaaki Ochi
    • Yo TaniguchiHisaaki Ochi
    • G01V3/00
    • G01R33/5613A61B5/055G01R33/543G01R33/586
    • The MRI apparatus of the present invention executes a non-imaging mode 501 for obtaining a steady state of magnetization and an imaging mode 502 for measuring echoes for images. In the non-imaging mode 501 and the imaging mode 502, imaging is performed by using a GrE type pulse sequence. In the imaging, RF pulses are irradiated while flip angle of nuclear magnetization in the imaging mode 502 is changed in a range of values not larger than a certain value determined by flip angle of nuclear magnetization used in the non-imaging mode 502 is irradiated. This certain value is, for example, the maximum value of flip angle of nuclear magnetization used in the non-imaging mode, or flip angle provided by an RF pulse used at the end of the non-imaging mode. SAR observed with use of a GrE type pulse sequence can be thereby reduced without degrading image contrast, and thus influence on human bodies can be reduced.
    • 本发明的MRI装置执行用于获得稳定的磁化状态的非成像模式501和用于测量图像的回波的成像模式502。 在非成像模式501和成像模式502中,通过使用GrE型脉冲序列进行成像。 在成像中,照射成像模式502中的核磁化的翻转角的RF脉冲在不大于由非成像模式502中使用的核磁化的翻转角确定的某个值的范围内变化的范围内。 该特定值例如是在非成像模式中使用的核磁化的翻转角的最大值或由在非成像模式结束时使用的RF脉冲提供的翻转角。 可以通过使用GrE型脉冲序列观察到的SAR,而不会降低图像对比度,从而可以降低对人体的影响。
    • 16. 发明授权
    • Magnetic resonance imaging apparatus
    • 磁共振成像装置
    • US07701214B2
    • 2010-04-20
    • US11912763
    • 2006-02-23
    • Shinji KurokawaYo TaniguchiHisaaki OchiShin-ichiro Umemura
    • Shinji KurokawaYo TaniguchiHisaaki OchiShin-ichiro Umemura
    • G01V3/00
    • G01R33/56375G01R33/56383
    • When a magnetic resonance signal is received more than once, while a table (transfer unit) is moved, a gradient magnetic field is applied in the table moving direction, and an application amount (intensity and application time) of the gradient magnetic field in the table moving direction is changed every acquisition of data. As for the encoding by the gradient magnetic field in the table moving direction, a series of phase encode is performed at different positions of an examination target, unlike a conventional phase encode. Therefore, the Fourier transform cannot be applied to the image reconstruction. Given this situation, a magnetization map of total FOV of the examination target is determined in such a manner that a sum of the square of an absolute value of a difference is minimized, the difference between a received signal and a signal calculated from the magnetization map set as a variable, and then, the reconstruction is performed. Even when a size of signal acquisition area in the table moving direction is narrow, the magnetic resonance imaging apparatus of the present invention is capable of taking an image of a wide field of view at high speed, by performing the imaging while the table is moved continuously.
    • 当多次接收到磁共振信号时,在移动台(传送单元)的同时,在台移动方向上施加梯度磁场,并且在梯形磁场的施加量(强度和施加时间) 每次采集数据时,表移动方向都会发生变化。 对于表移动方向的梯度磁场的编码,与现有的相位编码不同,在检查对象的不同位置进行一系列的相位编码。 因此,傅里叶变换不能应用于图像重构。 考虑到这种情况,检测对象的总FOV的磁化映射以如下方式来确定,使得差的绝对值的平方和之和最小化,接收信号与从磁化映射计算的信号之间的差 设置为变量,然后进行重建。 即使当表移动方向上的信号获取区域的尺寸窄时,本发明的磁共振成像装置也能够通过在桌子移动时进行成像而以高速拍摄宽视野的图像 不断地
    • 17. 发明申请
    • Magnetic Resonance Imaging Apparatus
    • 磁共振成像仪
    • US20090251142A1
    • 2009-10-08
    • US12308186
    • 2007-06-12
    • Yo TaniguchiHisaaki Ochi
    • Yo TaniguchiHisaaki Ochi
    • G01R33/54G01R33/28
    • G01R33/5613A61B5/055G01R33/543G01R33/586
    • The MRI apparatus of the present invention executes a non-imaging mode 501 for obtaining a steady state of magnetization and an imaging mode 502 for measuring echoes for images. In the non-imaging mode 501 and the imaging mode 502, imaging is performed by using a GrE type pulse sequence. In the imaging, RF pulses are irradiated while flip angle of nuclear magnetization in the imaging mode 502 is changed in a range of values not larger than a certain value determined by flip angle of nuclear magnetization used in the non-imaging mode 502 is irradiated. This certain value is, for example, the maximum value of flip angle of nuclear magnetization used in the non-imaging mode, or flip angle provided by an RF pulse used at the end of the non-imaging mode. SAR observed with use of a GrE type pulse sequence can be thereby reduced without degrading image contrast, and thus influence on human bodies can be reduced.
    • 本发明的MRI装置执行用于获得稳定的磁化状态的非成像模式501和用于测量图像的回波的成像模式502。 在非成像模式501和成像模式502中,通过使用GrE型脉冲序列进行成像。 在成像中,照射成像模式502中的核磁化的翻转角的RF脉冲在不大于由非成像模式502中使用的核磁化的翻转角确定的某个值的范围内变化的范围内。 该特定值例如是在非成像模式中使用的核磁化的翻转角的最大值或由在非成像模式结束时使用的RF脉冲提供的翻转角。 可以通过使用GrE型脉冲序列观察到的SAR,而不会降低图像对比度,从而可以降低对人体的影响。
    • 20. 发明申请
    • MAGNETIC RESONANCE IMAGING APPARATUS
    • 磁共振成像装置
    • US20090219020A1
    • 2009-09-03
    • US11912763
    • 2006-02-23
    • Shinji KurokawaYo TaniguchiHisaaki OchiShin-ichiro Umemura
    • Shinji KurokawaYo TaniguchiHisaaki OchiShin-ichiro Umemura
    • A61B5/055G01R33/20
    • G01R33/56375G01R33/56383
    • When a magnetic resonance signal is received more than once, while a table (transfer unit) is moved, a gradient magnetic field is applied in the table moving direction, and an application amount (intensity and application time) of the gradient magnetic field in the table moving direction is changed every acquisition of data. As for the encoding by the gradient magnetic field in the table moving direction, a series of phase encode is performed at different positions of an examination target, unlike a conventional phase encode. Therefore, the Fourier transform cannot be applied to the image reconstruction. Given this situation, a magnetization map of total FOV of the examination target is determined in such a manner that a sum of the square of an absolute value of a difference is minimized, the difference between a received signal and a signal calculated from the magnetization map set as a variable, and then, the reconstruction is performed. Even when a size of signal acquisition area in the table moving direction is narrow, the magnetic resonance imaging apparatus of the present invention is capable of taking an image of a wide field of view at high speed, by performing the imaging while the table is moved continuously.
    • 当多次接收到磁共振信号时,在移动台(传送单元)的同时,在台移动方向上施加梯度磁场,并且在梯形磁场的施加量(强度和施加时间) 每次采集数据时,表移动方向都会发生变化。 对于表移动方向的梯度磁场的编码,与现有的相位编码不同,在检查对象的不同位置进行一系列的相位编码。 因此,傅里叶变换不能应用于图像重构。 考虑到这种情况,检测对象的总FOV的磁化映射以如下方式来确定,使得差的绝对值的平方和之和最小化,接收信号与从磁化映射计算的信号之间的差 设置为变量,然后进行重建。 即使当表移动方向上的信号获取区域的尺寸窄时,本发明的磁共振成像装置也能够通过在桌子移动时进行成像而以高速拍摄宽视野的图像 不断地