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    • 4. 发明申请
    • Method and magnetic resonance tomography apparatus for spatially resolved measurement of the B1 field distribution
    • 用于B1场分布的空间分辨测量的方法和磁共振断层摄影装置
    • US20050073304A1
    • 2005-04-07
    • US10921606
    • 2004-08-19
    • Thorsten FeiweierPeter Heubes
    • Thorsten FeiweierPeter Heubes
    • G01R33/58G01V3/00
    • G01R33/583
    • In a method and magnetic resonance tomography apparatus for spatially resolved measurement of the magnetic high frequency field distribution in the apparatus, a double echo high frequency pulse sequence with a first excitation pulse following by at least two refocusing pulses are emitted for generation of a first echo and a following second echo. At least the excitation pulse is slice selective. In an excitation layer defined by the slice selective excitation pulse a first echo image and second echo image are spatially resolved by using suitable gradient pulses for phase or frequency encoding Using the relationships of the amplitudes of the first and second echo image in the various locations the flip angles representing the field strength at the relevant locations in the relevant slice are determined.
    • 在用于设备中的磁性高频场分布的空间分辨测量的方法和磁共振断层摄影装置中,发射具有随后至少两个重聚焦脉冲的第一激励脉冲的双回波高频脉冲序列,用于产生第一回波 和第二个回声。 至少激励脉冲是片选择性的。 在由切片选择性激发脉冲限定的激发层中,通过使用用于相位或频率编码的合适的梯度脉冲来对第一回波图像和第二回波图像进行空间分辨。使用各个位置中的第一和第二回波图像的振幅的关系, 确定表示相关切片中的相关位置处的场强的翻转角。
    • 5. 发明申请
    • Magnetic resonance tomography method and apparatus with suppression of ambiguity artifacts in spin echo images
    • 磁共振断层扫描方法和装置,其抑制自旋回波图像中的模糊伪像
    • US20050017719A1
    • 2005-01-27
    • US10898495
    • 2004-07-23
    • Peter Heubes
    • Peter Heubes
    • G01R33/48A61B5/055G01R33/565G01V3/00
    • G01R33/56563
    • In a magnetic resonance tomography method and apparatus for avoiding peripheral interference signals in magnetic resonance tomography when using spin-echo sequences, the average frequency and the bandwidth of the radio-frequency excitation pulse differ from the average frequency and the bandwidth of the radio-frequency refocusing pulse(s), and the amplitude of the slice selection gradients activated during the radio-frequency excitation pulse differing from the amplitude of the slice selection gradient(s) activated during the radio-frequency refocusing pulse, such that the excitation slice of the RF excitation pulse and the refocusing slice of the RF refocusing pulse(s) in the homogeneous volume (FOV) of the basic magnetic field are superimposed, while the excitation slice of the RF refocusing pulse(s) in the non-homogeneous volume of the basic magnetic field are separated locally, and an echo signal is thereby prevented in the non-homogeneous volume.
    • 在使用自旋回波序列的磁共振断层摄影中,用于避免磁共振断层摄影中的周边干扰信号的磁共振断层摄影方法和装置中,射频激励脉冲的平均频率和带宽不同于射频的平均频率和带宽 重聚焦脉冲,以及在射频激励脉冲期间激活的切片选择梯度的幅度与在射频重聚焦脉冲期间激活的切片选择梯度的幅度不同,使得激光切片 RF激励脉冲和基本磁场的均匀体积(FOV)中的RF重聚焦脉冲的重聚焦片叠加,同时在非均匀体积的RF重聚焦脉冲的激发切片 基本磁场被局部分离,从而在非均匀体积中防止回波信号。
    • 9. 发明授权
    • Method and magnetic resonance system for adjustment of the field strength of RF pulses
    • 用于调整RF脉冲场强的方法和磁共振系统
    • US07573266B2
    • 2009-08-11
    • US11612802
    • 2006-12-19
    • Thorsten FeiweierPeter HeubesThorsten Speckner
    • Thorsten FeiweierPeter HeubesThorsten Speckner
    • G01V3/00
    • G01R33/583G01R33/586
    • In a method for adjustment of the field strength of radio-frequency pulses as well as a magnetic resonance measurement system, radio-frequency pulses are emitted by a radio-frequency antenna of a magnetic resonance measurement system in a magnetic resonance measurement. A test volume slice is initially excited by emission of radio-frequency pulses with a defined pulse amplitude by the appertaining radio-frequency antenna and one-dimensional, spatially-resolved characteristic values are determined along an extent direction of the test volume slice. The one-dimensional, spatially-resolved characteristic values respectively represent a local field strength of the B1 field in strips of the test volume slice running perpendicular to the extent direction. An average value of the determined characteristic values is then formed over at least over one determined segment along the extent direction of the test volume slice. A pulse amplitude of the radio-frequency pulses that is to be set for the magnetic resonance measurement to be implemented is determined on the basis of the average value.
    • 在用于调整射频脉冲的场强的方法以及磁共振测量系统中,由磁共振测量系统的射频天线在磁共振测量中发射射频脉冲。 最初通过用相应的射频天线发射具有定义的脉冲幅度的射频脉冲来激发测试体积片,并且沿着测试体积片的范围方向确定一维的空间分辨特征值。 一维空间分辨特征值分别表示垂直于范围方向运行的测试体积切片中的B1场的局部场强。 然后,沿着测试体积切片的扩展方向在至少一个确定的段上形成所确定的特征值的平均值。 基于平均值来确定要实现的磁共振测量要设置的射频脉冲的脉冲幅度。
    • 10. 发明申请
    • METHOD AND MAGNETIC RESONANCE SYSTEM FOR ADJUSTMENT OF THE FIELD STRENGTH OF RF PULSES
    • 用于调整射频脉冲场强度的方法和磁共振系统
    • US20070145975A1
    • 2007-06-28
    • US11612802
    • 2006-12-19
    • Thorsten FeiweierPETER HEUBESTHORSTEN SPECKNER
    • Thorsten FeiweierPETER HEUBESTHORSTEN SPECKNER
    • G01V3/00
    • G01R33/583G01R33/586
    • In a method for adjustment of the field strength of radio-frequency pulses as well as a magnetic resonance measurement system, radio-frequency pulses are emitted by a radio-frequency antenna of a magnetic resonance measurement system in a magnetic resonance measurement A test volume slice is initially excited by emission of radio-frequency pulses with a defined pulse amplitude by the appertaining radio-frequency antenna and one-dimensional, spatially-resolved characteristic values are determined along an extent direction of the test volume slice. The one-dimensional, spatially-resolved characteristic values respectively represent a local field strength of the B1 field in strips of the test volume slice running perpendicular to the extent direction. An average value of the determined characteristic values is then formed over at least over one determined segment along the extent direction of the test volume slice. A pulse amplitude of the radio-frequency pulses that is to be set for the magnetic resonance measurement to be implemented is determined on the basis of the average value.
    • 在用于调整射频脉冲的场强的方法以及磁共振测量系统中,通过磁共振测量系统的射频天线在磁共振测量A中发射射频脉冲。测试体积切片 最初由具有定位的脉冲幅度的射频脉冲的发射激发,并且沿测试体积切片的范围方向确定一维的空间分辨特征值。 一维空间分辨特征值分别表示垂直于范围方向延伸的测试体积片的条带中的B SUB场的局部场强。 然后,沿着测试体积切片的扩展方向在至少一个确定的段上形成所确定的特征值的平均值。 基于平均值来确定要实现的磁共振测量要设置的射频脉冲的脉冲幅度。