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    • 1. 发明授权
    • Algorithm for adiabatic pulse design using the Shinnar Le-Roux transform
    • 使用Shinnar Le-Roux变换的绝热脉冲设计算法
    • US08473536B2
    • 2013-06-25
    • US12489285
    • 2009-06-22
    • Priti BalchandaniJohn M. PaulyDaniel M. Spielman
    • Priti BalchandaniJohn M. PaulyDaniel M. Spielman
    • G06F15/00G06F7/00
    • G01R33/44G01R33/4833
    • A method for providing an adiabatic RF pulse that is an inversion or refocusing pulse for a RF pulse sequence is provided. A linear phase frequency profile (Flp(ω)) is determined for the adiabatic RF pulse. A quadratic phase is applied to the linear phase frequency profile for the adiabatic RF pulse to obtain F(ω), wherein the applying the quadratic phase comprises setting F(ω)=Flp(ω)eikω2. A polynomial β is set to equal a Fourier Transform (F(ω)). A corresponding minimum phase α polynomial is determined for the β polynomial. (α,β) are set as inputs to an inverse Shinnar Le-Roux transform to generate an adiabatic RF waveform. The adiabatic RF waveform is truncated to produce the adiabatic RF pulse, wherein k>0.03π/(ω5−ωp)/(N+1) and k
    • 提供了一种用于提供作为RF脉冲序列的反转或重聚焦脉冲的绝热RF脉冲的方法。 确定绝热RF脉冲的线性相位频率分布(Flp(ω))。 将二次相位施加到用于绝热RF脉冲的线性相位频率分布以获得F(ω),其中应用二次相位包括设置F(ω)= Flp(ω)eikomega2。 多项式β被设置为等于傅里叶变换(F(ω))。 对于β多项式确定相应的最小相位α多项式。 (α,β)被设置为反向Shinnar Le-Roux变换的输入以产生绝热RF波形。 绝热RF波形被截断以产生绝热射频脉冲,其中k> 0.03pi /(ω5-omegap)/(N + 1)和k
    • 2. 发明授权
    • Self-refocused spatial-spectral pulse
    • 自重聚焦空间光谱脉冲
    • US07821263B2
    • 2010-10-26
    • US12136319
    • 2008-06-10
    • Priti BalchandaniDaniel SpielmanJohn M. Pauly
    • Priti BalchandaniDaniel SpielmanJohn M. Pauly
    • G01V3/00
    • G01R33/5601G01R33/4833G01R33/4835
    • A method for frequency selective and slice selective magnetic resonance imaging (MRI) is provided. A B0 field is applied. A self-refocused spatial-spectral (SPSP) RF pulse is applied. A readout of a portion of k-space for the excited slice is performed. A second self-refocused SPSP excitation RF pulse is applied, wherein the second self-refocused SPSP excitation has an 180° echo phase difference from the self-refocused SPSP excitation. A second readout of a portion of k-space for the excited slice was performed. A difference between the readout and the second readout was found. The previous steps were repeated until k-space has been filled for the excited slice. The previous steps were repeated for a plurality of slices.
    • 提供了频率选择和切片选择性磁共振成像(MRI)的方法。 应用B0字段。 应用自重聚焦空间光谱(SPSP)RF脉冲。 执行激励切片的k空间的一部分的读出。 应用第二个自重新聚焦的SPSP激励RF脉冲,其中第二自重聚焦SPSP激发与自重新聚焦的SPSP激发具有180°的回波相位差。 进行激发切片的k空间的一部分的第二次读出。 发现读出和第二读数之间的差异。 重复前面的步骤,直到激活切片填充k空间为止。 对于多个切片重复前面的步骤。
    • 3. 发明申请
    • SELF-REFOCUSED SPATIAL-SPECTRAL PULSE
    • 自反射空间光谱脉冲
    • US20090315558A1
    • 2009-12-24
    • US12136319
    • 2008-06-10
    • Priti BalchandaniDaniel SpielmanJohn M. Pauly
    • Priti BalchandaniDaniel SpielmanJohn M. Pauly
    • G01R33/48
    • G01R33/5601G01R33/4833G01R33/4835
    • A method for frequency selective and slice selective magnetic resonance imaging (MRI) is provided. A B0 field is applied. A self-refocused spatial-spectral (SPSP) RF pulse is applied. A readout of a portion of k-space for the excited slice is performed. A second self-refocused SPSP excitation RF pulse is applied, wherein the second self-refocused SPSP excitation has an 180° echo phase difference from the self-refocused SPSP excitation. A second readout of a portion of k-space for the excited slice was performed. A difference between the readout and the second readout was found. The previous steps were repeated until k-space has been filled for the excited slice. The previous steps were repeated for a plurality of slices.
    • 提供了频率选择和切片选择性磁共振成像(MRI)的方法。 应用B0字段。 应用自重聚焦空间光谱(SPSP)RF脉冲。 执行激励切片的k空间的一部分的读出。 应用第二个自重新聚焦的SPSP激励RF脉冲,其中第二自重聚焦SPSP激发与自重新聚焦的SPSP激发具有180°的回波相位差。 进行激发切片的k空间的一部分的第二次读出。 发现读出和第二读数之间的差异。 重复前面的步骤,直到激活切片填充k空间为止。 对于多个切片重复前面的步骤。
    • 4. 发明授权
    • Apparatus and method for rare echo imaging using k-space spiral coverage
    • 使用k空间螺旋覆盖的稀有回波成像的装置和方法
    • US5402067A
    • 1995-03-28
    • US101865
    • 1993-08-04
    • John M. PaulyDaniel M. SpielmanCraig H. MeyerAlbert MacovskiNorbert J. Pelc
    • John M. PaulyDaniel M. SpielmanCraig H. MeyerAlbert MacovskiNorbert J. Pelc
    • G01R33/20A61B5/055G01R33/48G01R33/561G01V3/00
    • G01R33/5615G01R33/446G01R33/5617
    • A long train of spin echoes is produced using a RARE excitation pulse sequence, and during each spin echo an annular segment of a long k-space spiral as determined by read-out magnetic gradients is detected. At the end of the echo train the entire k-space spiral will have been covered. Each of the segments can be a unique annular portion of the k-space spiral. Alternatively, fewer annular segments of the spiral can be provided, with the fewer annular segments rotated in k-space and replayed to cover interleaved paths in k-space. The imaging gradients are refocused at the time of each spin-echo pulse in order to permit the long echo pulse trains of RARE imaging. Each spiral segment is surrounded by gradient lobes that move out from the k-space origin to the beginning of the segment, and move back to the origin from the end of the segment. Advantageously, the magnetic gradient lobes can be produced concurrently with parasitic echo crusher gradients at the beginning and end of each spin-echo pulse. Further, off-resonance effects can be placed in sidelobes of the spin-echo signal to facilitate suppression in the detected signals.
    • 使用RARE激励脉冲序列产生长串自旋回波,并且在每个自旋回波期间,检测由读出磁梯度确定的长k空间螺旋的环形段。 在回波列车的末端,整个k空间螺旋将被覆盖。 每个段可以是k空间螺旋的独特的环形部分。 或者,可以提供更少的螺旋环形段,其中较少的环形段在k空间中旋转并且重播以覆盖k空间中的交错路径。 在每个自旋回波脉冲时,成像梯度被重新聚焦,以便允许RARE成像的长回波脉冲序列。 每个螺旋段由从k空间原点移出到段的开头的梯度波瓣包围,并从段的末尾返回到原点。 有利地,可以在每个自回波脉冲的开始和结束处与寄生回波破碎机梯度同时产生磁梯度波瓣。 此外,离共振效应可以置于自旋回波信号的旁瓣中,以便于检测信号中的抑制。