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    • 1. 发明授权
    • Method of MR (=magnetic resonance) with spatial encoding to generate an image or spectroscopic data
    • 使用空间编码的MR(=磁共振)方法来生成图像或光谱数据
    • US08791700B2
    • 2014-07-29
    • US13137086
    • 2011-07-20
    • Walter WitscheyDaniel GallichanMaxim ZaitsevGerrit SchultzJuergen Hennig
    • Walter WitscheyDaniel GallichanMaxim ZaitsevGerrit SchultzJuergen Hennig
    • G01V3/00G01R33/44
    • G01R33/445G01R33/4833
    • A method of MR with spatial encoding to generate an image or spectroscopic data of an object of investigation inside an MR apparatus comprises the steps of (a) selecting a volume of interest within the object of investigation, (b) applying an RF pulse to generate a transverse magnetization within the object of investigation, (c) preparing a nonlinear phase distribution within the object of investigation by application of spatially encoding magnetic fields (SEMs), the SEMs comprising of a nonlinear gradient field or a combination of linear and nonlinear gradient fields, (d) effecting primary spatial encoding through application of SEMs, and (e) recording MR signals originating from the object of investigation. Step (c) or (d) thereby comprises applying a sequence of at least two SEMs, at least one of which contains a nonlinear field gradient and at least two of the SEMs having different field geometries. The sequence of SEMs is applied at a point in time from and including the excitation of the object of interest in step (b) up to and including the recording of the MR signals in step (e), to thereby introduce a temporal shift of the signals arising from spatially different locations within the selected volume of interest, that is to thereby introduce a shift of local spatial frequency components. A sampling window for recording of the respective MR signals is set and signals originating from the volume of interest are recorded in step (e) and undesired signals originating from outside the volume of interest are suppressed.
    • 一种具有空间编码以在MR装置内产生调查对象的图像或光谱数据的MR的方法包括以下步骤:(a)选择调查对象内的感兴趣体积,(b)施​​加RF脉冲以产生 在研究对象内的横向磁化,(c)通过应用空间编码磁场(SEM)在研究对象内准备非线性相位分布,包括非线性梯度场或线性和非线性梯度场的组合的SEM ,(d)通过应用SEM实现主要空间编码,(e)记录源自调查对象的MR信号。 步骤(c)或(d)由此包括施加至少两个SEM序列,其中至少一个包含非线性场梯度和具有不同场几何形状的至少两个SEM。 在从步骤(b)中的感兴趣对象的激发到包括步骤(e)中的MR信号的记录的时间点上施加SEM序列,从而引入时间偏移 在所选择的感兴趣体积内由空间不同的位置产生的信号,从而引入局部空间频率分量的偏移。 设置用于记录各个MR信号的采样窗口,并且在步骤(e)中记录来自感兴趣体积的信号,并且抑制源于感兴趣体积之外的不需要的信号。
    • 2. 发明授权
    • Method for position dependent change in the magnetization in an object in a magnetic resonance experiment
    • 磁共振实验中物体磁化位置相关变化的方法
    • US08508227B2
    • 2013-08-13
    • US12897806
    • 2010-10-05
    • Martin HaasPeter UllmannWolfgang RuhmMaxim ZaitsevJürgen Hennig
    • Martin HaasPeter UllmannWolfgang RuhmMaxim ZaitsevJürgen Hennig
    • G01V3/00
    • G01R33/4836G01R33/3415G01R33/385G01R33/4833G01R33/5612
    • A method for position dependent change in the magnetization in an object, according to a requirement in a magnetic resonance measurement, wherein radio-frequency pulses are irradiated in conjunction with supplementary magnetic fields that vary in space and over time and are superposed on the static and homogeneous basic field of a magnetic resonance measurement apparatus along a z-direction, is characterized in that non-linear supplementary magnetic fields are used, whose spatial gradient of the z-component is not constant at least at one instant of the irradiation, and that the radio-frequency pulses to be irradiated are calculated in advance, wherein progressions over time of the field strengths of the supplementary magnetic fields in the region of the object that are calculated and/or measured position-dependently are included in this calculation. This enables change in the magnetization with an at least locally spatially higher resolution and/or shorter irradiation duration of the RF pulses and supplementary magnetic fields than is feasible with linear supplementary magnetic fields produced by conventional gradient systems. In particular, this is possible under the technical and physiological conditions that currently constrain the performance of the known methods using linear supplementary fields.
    • 根据磁共振测量中的要求,对物体的磁化位置相关变化的方法,其中射频脉冲与空间和时间上变化并叠加在静态和 磁共振测量装置沿z方向的均匀基本场的特征在于,使用非线性辅助磁​​场,其至少在照射一瞬间z分量的空间梯度不恒定,并且 预先计算要照射的射频脉冲,其中在该计算中包括在计算和/或测量的对象的区域中的辅助磁场的场强随时间的逐渐增加。 这使得能够利用由常规梯度系统产生的线性补充磁场可行的RF脉冲和辅助磁场的至少局部空间上更高的分辨率和/或更短的照射持续时间来改变磁化。 特别地,这在目前限制使用线性补充领域的已知方法的性能的技术和生理条件下是可能的。
    • 3. 发明申请
    • Method of dynamically compensating for magnetic field heterogeneity in magnetic resonance imaging
    • 动态补偿磁共振成像磁场异质性的方法
    • US20120249137A1
    • 2012-10-04
    • US13414737
    • 2012-03-08
    • Walter WitscheyMaxim ZaitsevJürgen HennigGerrit SchultzDaniel Gallichan
    • Walter WitscheyMaxim ZaitsevJürgen HennigGerrit SchultzDaniel Gallichan
    • G01R33/58
    • G01R33/3875
    • A method to compensate for the magnetic field heterogeneity inside an object of investigation in a MR device obtains an uncorrected magnetic field distribution of the object and executes an MR sequence with a desired k-space coverage by applying RF pulses to generate a transverse magnetization within the object. MR signal data is recorded, magnetic field shimming parameters are dynamically updated and MR signal data are reconstructed to produce images or localized spectroscopic data. Artifacts in a reconstructed image resulting from an uncorrected magnetic field distribution are suppressed by temporally separating MR signals originating from at least two different sub-volumes within a volume of transverse magnetization by generating a nonlinear phase distribution within the object and by dynamically updating shimming parameters to compensate for the field inhomogeneity distributions within the different sub-volumes in the volume of transverse magnetization.
    • 用于补偿MR装置内的调查对象内的磁场异质性的方法获得对象的未校正的磁场分布,并通过施加RF脉冲来产生具有期望的k空间覆盖的MR序列,以在其内产生横向磁化 目的。 记录MR信号数据,动态地更新磁场匀场参数,重建MR信号数据以产生图像或局部光谱数据。 通过在对象内生成非线性相位分布,并且通过动态地更新匀场参数来暂时分离来自横向磁化体积内的至少两个不同子体积的MR信号,从而抑制由未校正的磁场分布产生的重构图像中的人造物 补偿横向磁化量的不同子体积内的场不均匀性分布。
    • 4. 发明授权
    • Magnetic resonance selective excitation method of a target distribution of magnetization with complete full integration of bloch equations for RF large angle pulses (LAP)'s that are 15 degrees or greater, without small angle approximation
    • 磁共振选择激励方法的目标磁化分布方法,对于大于15度或更大的RF大角度脉冲(LAP)的完全整体积分,无小角度逼近
    • US08368400B2
    • 2013-02-05
    • US12382202
    • 2009-03-11
    • Martin HaasMaxim ZaitsevJürgen Hennig
    • Martin HaasMaxim ZaitsevJürgen Hennig
    • G01V3/00
    • G01R33/483G01R33/4833G01R33/4836G01R33/543G01R33/5611G01R33/5612G01R33/5613G01R33/5617
    • A magnetic resonance method for using radio frequency pulses for spatially selective and frequency selective or multidimensionally spatially selective excitation of an ensemble of nuclear spins with an initial distribution of magnetization in a main magnetic field aligned along a z-axis, wherein a spin magnetization with a given target distribution of magnetization is generated, and for refocusing the spin magnetization, is characterized in that the radio frequency pulse is used as a sequence of sub-pulses of independent duration, courses of gradients and spatial and/or spectral resolution, comprising one or more large angle RF pulses with tip angles greater than or approximately equal to 15°, which generate a gross distribution of magnetization approximating the target distribution of magnetization or a desired modification of the distribution of magnetization with a mean deviation less than or approximately equal to 15°, wherein the actual effect of the LAPs on the distribution of spin magnetization before the radio frequency pulse is used is calculated by integration of the Bloch equations without small angle approximation, and one or more small angle RF pulses=SAPs with tip angles less than or approximately equal to 15° reducing the difference between the target distribution of magnetization and the gross distribution of magnetization caused by the LAPs.
    • 一种磁共振方法,用于使用射频脉冲用于沿着z轴对准的主磁场中的初始磁化分布的核自旋组合的空间选择性或频率选择性或多维空间选择性激发,其中自旋磁化与 产生磁化的目标分布,并且对于重新聚焦自旋磁化,其特征在于射频脉冲被用作独立持续时间,梯度,空间和/或光谱分辨率的子脉冲序列,包括一个或 具有大于或大约等于15°的尖角的更大的角度RF脉冲,其产生近似磁化的目标分布的磁化的总体分布或磁化分布的期望修改,平均偏差小于或等于15 °,其中LAP对分布的实际效果 使用无线电频率脉冲之前的自旋磁化是通过不使用小角度近似的Bloch方程的积分计算的,并且一个或多个小角度RF脉冲=具有小于或等于15°的尖角的SAP减少目标分布之间的差异 的磁化和由LAP引起的磁化的总分布。
    • 5. 发明授权
    • Method for data acquisition acceleration in magnetic resonance imaging (MRI) with N-dimensional spatial encoding using two or more receiver coil arrays and non-linear phase distributions
    • 使用两个或多个接收器线圈阵列和非线性相位分布进行N维空间编码的磁共振成像(MRI)中的数据采集加速方法
    • US08354844B2
    • 2013-01-15
    • US12645505
    • 2009-12-23
    • Maxim ZaitsevJuergen Hennig
    • Maxim ZaitsevJuergen Hennig
    • G01V3/00
    • G01R33/5611G01R33/4836
    • A method for accelerating data acquisition in MRI with N-dimensional spatial encoding has a first method step in which a transverse magnetization within an imaged object volume is prepared having a non-linear phase distribution. Primary spatial encoding is thereby effected through application of switched magnetic fields. Two or more RF receivers are used to simultaneously record MR signals originating from the imaged object volume, wherein, for each RF receiver, an N-dimensional data matrix is recorded which is undersampled by a factor Ri per selected k-space direction. Data points belonging to a k-space matrix which were not recoded by a selected acquisition schema are reconstructed using a parallel imaging method, wherein reference information concerning receiver coil sensitivities is extracted from a phase-scrambled reconstruction of the undersampled data matrix. The method generates a high-resolution image free of artifacts in a time-efficient manner by improving data sampling efficiency and thereby reducing overall data acquisition time.
    • 用于加速具有N维空间编码的MRI中的数据采集的方法具有第一方法步骤,其中准备具有非线性相位分布的成像对象体积内的横向磁化强度。 从而通过应用开关磁场来实现主空间编码。 使用两个或更多个RF接收器来同时记录来自成像对象体积的MR信号,其中,对于每个RF接收机,记录N个数据矩阵,其被每个选择的k空间方向的因子Ri欠采样。 使用并行成像方法重建属于未被所选择的采集模式重新编码的k空间矩阵的数据点,其中关于接收机线圈灵敏度的参考信息是从欠采样数据矩阵的相位加扰重建中提取的。 该方法通过提高数据采样效率从而减少总体数据采集时间,以时间有效的方式产生无瑕疵的高分辨率图像。
    • 7. 发明申请
    • Method for position dependent change in the magnetization in an object in a magnetic resonance experiment
    • 磁共振实验中物体磁化位置相关变化的方法
    • US20110080169A1
    • 2011-04-07
    • US12897806
    • 2010-10-05
    • Martin HaasPeter UllmannWolfgang RuhmMaxim ZaitsevJürgen Hennig
    • Martin HaasPeter UllmannWolfgang RuhmMaxim ZaitsevJürgen Hennig
    • G01R33/48
    • G01R33/4836G01R33/3415G01R33/385G01R33/4833G01R33/5612
    • A method for position dependent change in the magnetization in an object, according to a requirement in a magnetic resonance measurement, wherein radio-frequency pulses are irradiated in conjunction with supplementary magnetic fields that vary in space and over time and are superposed on the static and homogeneous basic field of a magnetic resonance measurement apparatus along a z-direction, is characterized in that non-linear supplementary magnetic fields are used, whose spatial gradient of the z-component is not constant at least at one instant of the irradiation, and that the radio-frequency pulses to be irradiated are calculated in advance, wherein progressions over time of the field strengths of the supplementary magnetic fields in the region of the object that are calculated and/or measured position-dependently are included in this calculation. This enables change in the magnetization with an at least locally spatially higher resolution and/or shorter irradiation duration of the RF pulses and supplementary magnetic fields than is feasible with linear supplementary magnetic fields produced by conventional gradient systems. In particular, this is possible under the technical and physiological conditions that currently constrain the performance of the known methods using linear supplementary fields.
    • 根据磁共振测量中的要求,对物体的磁化位置相关变化的方法,其中射频脉冲与空间和时间上变化并叠加在静态和 磁共振测量装置沿z方向的均匀基本场的特征在于,使用非线性辅助磁​​场,其至少在照射一瞬间z分量的空间梯度不恒定,并且 预先计算要照射的射频脉冲,其中在该计算中包括在计算和/或测量的对象的区域中的辅助磁场的场强随时间的逐渐增加。 这使得能够利用由常规梯度系统产生的线性补充磁场可行的RF脉冲和辅助磁场的至少局部空间上更高的分辨率和/或更短的照射持续时间来改变磁化。 特别地,这在目前限制使用线性补充领域的已知方法的性能的技术和生理条件下是可能的。
    • 8. 发明授权
    • NMR tomography method based on NBSEM with 2D spatial encoding by two mutually rotated multipole gradient fields
    • 基于具有通过两个相互旋转的多极梯度场的2D空间编码的NBSEM的NMR层析成像方法
    • US07906968B2
    • 2011-03-15
    • US12291680
    • 2008-11-12
    • Juergen HennigMaxim ZaitsevAnna WelzGerrit Schultz
    • Juergen HennigMaxim ZaitsevAnna WelzGerrit Schultz
    • G01V3/00
    • G01R33/385G01R33/3415G01R33/3854G01R33/48
    • A nuclear magnetic resonance (NMR) imaging method in which, with the aid of a gradient system, a spatially and temporally variable magnetic field Bgrad is generated, for the at least two-dimensional spatial encoding of NMR measurement signals in a measurement sample region to be imaged, where the magnetic field Bgrad is employed in at least two forms Bgrad1 and Bgrad2 in the measurement sample region to be imaged during a single measurement cycle from excitation to reading of the NMR measurement signals, where the first form Bgrad1 has essentially ns poles, where ns is an even number > 2, and has ns essentially sectorial sub-regions, in each of which the magnetic field Bgrad is locally monotonic in one direction, where the measurement signals from the measurement sample are recorded by means of at least ns receiver coils which have different sensitivity over the ns sub-regions of the region to be imaged, is characterized in that the second form Bgrad2 is essentially identical to the first form Bgrad1 % with the second form Bgrad2 being rotated by an angle Δφ, where Δ ⁢ ⁢ φ = 360 ⁢ ° 2 · n ⁢ ⁢ s , relative to the first form Bgrad1. The invention provides an NMR imaging method in which a high-resolution image of the region to be imaged is obtained more quickly utilizing the advantages of NBSEMs.
    • 一种核磁共振(NMR)成像方法,其中借助于梯度系统产生空间和时间上可变的磁场Bgrad,对于测量样本区域中的NMR测量信号的至少二维空间编码, 成像,其中在从激励到读取NMR测量信号的单个测量周期期间在要成像的测量样本区域中至少两种形式Bgrad1和Bgrad2采用磁场Bgrad,其中第一形式Bgrad1具有基本上为ns的极点 ,其中ns是偶数> 2,并且具有基本上是扇形子区域,其中每个子场中的磁场Bgrad在一个方向上局部单调,其中来自测量样本的测量信号通过至少ns 具有与要成像的区域的ns子区域不同的灵敏度的接收器线圈的特征在于,第二形式Bgrad2基本上与fi 第一种形式Bgrad1%,第二种形式Bgrad2旋转角度&Dgr;&phgr;其中&Dgr; ⁢&phgr = 360°2·n⁢s,相对于第一形式Bgrad1。 本发明提供了一种NMR成像方法,其中使用NBSEM的优点更快地获得待成像区域的高分辨率图像。