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    • 4. 发明授权
    • Method for determining magnetic resonance data
    • 确定磁共振数据的方法
    • US08896307B2
    • 2014-11-25
    • US13422434
    • 2012-03-16
    • Jan Ole BlumhagenMatthias FenchelRalf Ladebeck
    • Jan Ole BlumhagenMatthias FenchelRalf Ladebeck
    • G01R33/44G01R33/565G01R33/48
    • G01R33/481G01R33/56563G01R33/56572
    • According to an embodiment of a method, a first readout gradient field is determined in such a way that a distortion caused by a non-linearity of the first readout gradient field and a distortion caused by a B0 field inhomogeneity are essentially cancelled at a first location of a field of view of the magnetic resonance facility. Moreover, a second readout gradient field is determined in such a way that a distortion caused by a non-linearity of the second readout gradient field and a distortion caused by a B0 field inhomogeneity are essentially cancelled at a different second location of the field of view. Finally, a multiecho sequence is performed, wherein first magnetic resonance data is captured using the first readout gradient field after a 180° pulse and second magnetic resonance data is captured using the second readout gradient field after a further 180° pulse.
    • 根据方法的实施例,第一读出梯度场被确定为使得由第一读出梯度场的非线性引起的失真和由B0场不均匀性引起的失真在第一位置处被基本上消除 的磁共振设备的视场。 此外,以这样的方式确定第二读出梯度场,使得由第二读出梯度场的非线性引起的失真和由B0场不均匀性引起的失真在视场的不同的第二位置基本上消除 。 最后,执行多电路序列,其中在180°脉冲之后使用第一读出梯度场捕获第一磁共振数据,并且在进一步180°脉冲之后使用第二读出梯度场捕获第二磁共振数据。
    • 8. 发明申请
    • METHOD FOR DETERMINING MAGNETIC RESONANCE DATA
    • 用于确定磁共振数据的方法
    • US20120235680A1
    • 2012-09-20
    • US13422434
    • 2012-03-16
    • Jan Ole BlumhagenMatthias FenchelRalf Ladebeck
    • Jan Ole BlumhagenMatthias FenchelRalf Ladebeck
    • G01R33/44
    • G01R33/481G01R33/56563G01R33/56572
    • According to an embodiment of a method, a first readout gradient field is determined in such a way that a distortion caused by a non-linearity of the first readout gradient field and a distortion caused by a B0 field inhomogeneity are essentially cancelled at a first location of a field of view of the magnetic resonance facility. Moreover, a second readout gradient field is determined in such a way that a distortion caused by a non-linearity of the second readout gradient field and a distortion caused by a B0 field inhomogeneity are essentially cancelled at a different second location of the field of view. Finally, a multiecho sequence is performed, wherein first magnetic resonance data is captured using the first readout gradient field after a 180° pulse and second magnetic resonance data is captured using the second readout gradient field after a further 180° pulse.
    • 根据方法的实施例,第一读出梯度场被确定为使得由第一读出梯度场的非线性引起的失真和由B0场不均匀性引起的失真在第一位置处被基本上消除 的磁共振设备的视场。 此外,以这样的方式确定第二读出梯度场,使得由第二读出梯度场的非线性引起的失真和由B0场不均匀性引起的失真在视场的不同的第二位置基本上消除 。 最后,执行多电路序列,其中在180°脉冲之后使用第一读出梯度场捕获第一磁共振数据,并且在进一步180°脉冲之后使用第二读出梯度场捕获第二磁共振数据。
    • 10. 发明申请
    • Background signal suppression in pet spectrums
    • 宠物光谱背景信号抑制
    • US20100108895A1
    • 2010-05-06
    • US12591003
    • 2009-11-04
    • Ralf LadebeckMarkus Vester
    • Ralf LadebeckMarkus Vester
    • G01T1/164
    • G01T1/00
    • A method and a facility are disclosed for imaging a PET spectrum with a PET detector, especially a PE-MR tomograph, and evaluation of the PET spectrum. To improve the correction of the base line in PET and thereby to improve the energy resolution for the PET images, at least one embodiment of the facility includes: a sampling facility for sampling the output signal of the PET detector at a predetermined sampling rate; an edge discriminator for recognizing at least one edge of a PET pulse; a background signal discriminator for estimating a background signal under the PET pulse; and an integrator device for determining the energy of the PET pulse in the PET spectrum above of the background signal from the sample values of the sampling facility.
    • 公开了一种利用PET检测器,特别是PE-MR断层摄影仪对PET光谱进行成像并评估PET光谱的方法和设备。 为了改善PET中基线的校正,从而提高PET图像的能量分辨率,设备的至少一个实施例包括:采样设备,用于以预定采样率对PET检测器的输出信号进行采样; 用于识别PET脉冲的至少一个边缘的边缘鉴别器; 背景信号鉴别器,用于估计PET脉冲下的背景信号; 以及积分器装置,用于根据来自采样设备的样本值的背景信号确定PET谱中PET脉冲的能量。