CN112557978B - Multi-echo sampling method based on three-dimensional non-Cartesian trajectory - Google Patents
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Abstract
本发明提供了一种基于三维非笛卡尔轨迹的多回波采样方法,用于定量磁化率成像技术,具体包括:选取圆柱形k空间,在所述圆柱形k空间内选取多个采集平面,并对所述多个采集平面进行编码;在所述多个采集平面中的每一个所述采集平面上,选取数据采集曲线;根据所述多个采集平面的编码以及每一个所述采集曲线确定三维非笛卡尔轨迹;根据所述三维非笛卡尔轨迹设计扫描时间序列;根据所述扫描时间序列,实施共振数据采集。本发明通过三维非笛卡尔轨迹,增加了k空间的填充率,提高了数据采集效率,缩短了定量磁化率成像时间。
The present invention provides a multi-echo sampling method based on a three-dimensional non-Cartesian trajectory for quantitative magnetic susceptibility imaging technology, which specifically includes: selecting a cylindrical k-space, selecting multiple acquisition planes in the cylindrical k-space, encoding the multiple acquisition planes; on each of the multiple acquisition planes, select a data acquisition curve; determine according to the encoding of the multiple acquisition planes and each of the acquisition curves Three-dimensional non-Cartesian trajectory; design a scan time sequence according to the three-dimensional non-Cartesian trajectory; implement resonance data acquisition according to the scan time series. Through the three-dimensional non-Cartesian trajectory, the invention increases the filling rate of the k-space, improves the data acquisition efficiency, and shortens the quantitative magnetic susceptibility imaging time.
Description
技术领域technical field
本发明属于定量磁化率成像的技术领域,尤其涉及一种基于三维非笛卡尔轨迹的多回波采样方法。The invention belongs to the technical field of quantitative magnetic susceptibility imaging, and in particular relates to a multi-echo sampling method based on a three-dimensional non-Cartesian trajectory.
背景技术Background technique
定量磁化率成像(Quantitative Susceptibility Mapping,QSM)是磁共振成像中用于生物组织磁化特性的三维定量可视化技术。磁化率是物质的一种固有物理属性,它反映物质在外磁场中的被磁化大小的能力。当磁化率源置于外磁场时,会引起局部的磁场变化,导致磁共振信号在多回波中有不同的相位递进。定量磁化率成像技术通过对图像相位的分析,使用逆问题求解的算法,对组织中的铁含量、钙化、血氧饱和度变化等生理现象造成的磁化率变化进行定量化测量。使用定量磁化率成像进行脑部成像,可以获得脑铁含量的空间分布,从而辅助检查脑出血、多发性硬化症以及帕金森综合征等疾病。Quantitative Susceptibility Mapping (QSM) is a three-dimensional quantitative visualization technique for the magnetic properties of biological tissues in magnetic resonance imaging. Magnetic susceptibility is an inherent physical property of matter, which reflects the ability of matter to be magnetized in an external magnetic field. When the magnetic susceptibility source is placed in an external magnetic field, it will cause local magnetic field changes, resulting in different phase progressions of the magnetic resonance signals in multiple echoes. Quantitative magnetic susceptibility imaging technology quantitatively measures the magnetic susceptibility changes caused by physiological phenomena such as iron content, calcification, and changes in blood oxygen saturation in tissues by analyzing the image phase and using the algorithm of inverse problem solving. Brain imaging using quantitative magnetic susceptibility imaging can obtain the spatial distribution of brain iron content, which can aid in the examination of diseases such as cerebral hemorrhage, multiple sclerosis, and Parkinson's syndrome.
在现有的定量磁化率成像技术中,对于多回波采样通常遵循笛卡尔轨迹。具体地,对于单次脉冲所激发的多个梯度回波信号,在k空间中填充笛卡尔轨迹,遵循笛卡尔轨迹采集这些回波信号。然而,笛卡尔轨迹在k空间中的填充率较低,导致数据采集效率较低,使得定量磁化率成像时间较长。以256个相位编码为例,采用传统笛卡尔轨迹采集时,在单次脉冲激发后仅填充k空间的一行数据,完成全部k空间的填充需要256次脉冲激发。相比于笛卡尔轨迹,采用非笛卡尔轨迹采集时,单次脉冲激发后可以填充的k空间范围更大,因此可以减少所需的脉冲激发次数,从而提高采集效率,缩短扫描时间。In existing quantitative susceptibility imaging techniques, a Cartesian trajectory is generally followed for multi-echo sampling. Specifically, for multiple gradient echo signals excited by a single pulse, a Cartesian trajectory is filled in k-space, and these echo signals are collected following the Cartesian trajectory. However, Cartesian trajectories have a low filling rate in k-space, resulting in inefficient data acquisition and long quantitative susceptibility imaging times. Taking 256 phase codes as an example, when using traditional Cartesian trajectory acquisition, only one row of data in k-space is filled after a single pulse excitation, and 256 pulse excitations are required to complete the filling of all k-space. Compared with the Cartesian trajectory, when the non-Cartesian trajectory is used for acquisition, the k-space range that can be filled after a single pulse excitation is larger, so the required pulse excitation times can be reduced, thereby improving the acquisition efficiency and shortening the scanning time.
因此,本领域技术人员期望研发一种基于三维非笛卡尔轨迹的多回波采样方法,以提高数据采集效率,从而缩短定量磁化率成像的时间。Therefore, those skilled in the art expect to develop a multi-echo sampling method based on three-dimensional non-Cartesian trajectories, so as to improve the efficiency of data acquisition, thereby shortening the time for quantitative magnetic susceptibility imaging.
发明内容SUMMARY OF THE INVENTION
本发明提供了一种基于三维非笛卡尔轨迹的多回波采样方法,具体包括以下步骤:The present invention provides a multi-echo sampling method based on a three-dimensional non-Cartesian trajectory, which specifically includes the following steps:
步骤1、选取圆柱形k空间,并在所述圆柱形k空间内选取多个采集平面,并对所述多个采集平面进行编码;Step 1, select a cylindrical k-space, and select a plurality of acquisition planes in the cylindrical k-space, and encode the plurality of acquisition planes;
步骤2、在所述多个采集平面中的每一个所述采集平面上,选取数据采集曲线;Step 2, on each of the multiple acquisition planes, select a data acquisition curve;
步骤3、根据所述多个采集平面的编码以及每一个所述采集曲线确定三维非笛卡尔轨迹;Step 3, determining a three-dimensional non-Cartesian trajectory according to the encoding of the multiple acquisition planes and each of the acquisition curves;
步骤4、根据所述三维非笛卡尔轨迹设计扫描时间序列;Step 4, designing a scanning time series according to the three-dimensional non-Cartesian trajectory;
步骤5、根据所述扫描时间序列,实施共振数据采集。Step 5, according to the scanning time sequence, implement resonance data acquisition.
进一步地,在步骤1中,所述多个采集平面呈互相平行。Further, in step 1, the multiple acquisition planes are parallel to each other.
进一步地,在步骤1中,所述多个采集平面均垂直于所述圆柱形k空间的选层方向。Further, in step 1, the multiple acquisition planes are all perpendicular to the slice selection direction of the cylindrical k-space.
进一步地,在步骤1中,所述多个采集平面采用等距编码以确定所述采集平面的选层方向坐标。Further, in step 1, equidistant coding is used for the multiple acquisition planes to determine the layer selection direction coordinates of the acquisition planes.
进一步地,所述等距编码满足如下关系式:Further, the equidistant coding satisfies the following relational formula:
其中,为第i次选层编码时的采集平面的选层方向坐标,Nz为所述圆柱形k空间选层方向上坐标的最大值,i为正整数,i=1,2,...,Nz。in, is the layer selection direction coordinates of the acquisition plane during the i-th layer selection encoding, N z is the maximum value of the coordinates in the layer selection direction of the cylindrical k-space, i is a positive integer, i=1, 2,..., N z .
进一步地,,在步骤1中,所述多个采集平面采用非等距编码以确定所述采集平面的选层方向坐标。Further, in step 1, non-equidistant coding is used for the multiple acquisition planes to determine the layer selection direction coordinates of the acquisition planes.
进一步地,所述非等距编码满足如下关系式:Further, the non-equidistant coding satisfies the following relational expression:
其中,γ为比例系数,mod()为取余运算,为第i次选层编码时的采集平面的选层方向坐标,Nz为所述圆柱形k空间选层方向上坐标的最大值,i为正整数,i=1,2,...,Nz。Among them, γ is the proportional coefficient, mod() is the remainder operation, is the layer selection direction coordinates of the acquisition plane during the i-th layer selection encoding, N z is the maximum value of the coordinates in the layer selection direction of the cylindrical k-space, i is a positive integer, i=1, 2,..., N z .
进一步地,所述比例系数γ满足如下关系式:Further, the proportional coefficient γ satisfies the following relational formula:
进一步地,在所述步骤2中,所述采集曲线为所述采集面上的采集坐标关于采集时间的函数。Further, in the step 2, the acquisition curve is a function of the acquisition coordinates on the acquisition surface and the acquisition time.
进一步地,所述采集曲线满足所述采集坐标周期性地等于所述采集平面的原点。Further, the acquisition curve satisfies that the acquisition coordinates are periodically equal to the origin of the acquisition plane.
相对于现有技术而言,本申请提供的基于三维非笛卡尔轨迹的多回波采样方法具有的技术效果为:在圆柱形k空间中选取了多个采集面以及非笛卡尔采集曲线,相比于笛卡尔轨迹,采用非笛卡尔轨迹采集时,单次脉冲激发后可以填充的k空间范围更大,因此可以减少所需的脉冲激发次数,从而提高采集效率,缩短扫描时间。对k空间的填充率高,提升了数据采样效率,以此缩短扫描时间,使得缩短定量磁化率成像所需时间显著减少。Compared with the prior art, the multi-echo sampling method based on the three-dimensional non-Cartesian trajectory provided by the present application has the technical effect of: selecting a plurality of acquisition surfaces and non-Cartesian acquisition curves in the cylindrical k-space, Compared with the Cartesian trajectory, when the non-Cartesian trajectory is used for acquisition, the k-space range that can be filled after a single pulse excitation is larger, so the required pulse excitation times can be reduced, thereby improving the acquisition efficiency and shortening the scanning time. The high filling rate of the k-space improves the data sampling efficiency, thereby shortening the scanning time and significantly reducing the time required for quantitative magnetic susceptibility imaging.
附图说明Description of drawings
图1是本申请的一个实施例的三维非笛卡尔轨迹在某一个采样平面中采样曲线示意图;1 is a schematic diagram of a sampling curve of a three-dimensional non-Cartesian trajectory in a certain sampling plane according to an embodiment of the present application;
图2是本申请的一个实施例的三维非笛卡尔轨迹示意图;2 is a schematic diagram of a three-dimensional non-Cartesian trajectory according to an embodiment of the present application;
图3是本申请的一个实施例的扫描时间序列示意图。FIG. 3 is a schematic diagram of a scanning time series according to an embodiment of the present application.
具体实施方式Detailed ways
以下参考说明书附图介绍本发明的实施例,使其技术内容更加清楚和便于理解。本发明可以通过许多不同形式的实施例来得以体现,本发明的保护范围并非仅限于文中提到的实施例。在本申请中,k空间为圆柱形空间。圆柱形k空间中的z方向为中心轴线方向,也被称为kz方向或选层编码方向。The following describes the embodiments of the present invention with reference to the accompanying drawings, so as to make its technical content clearer and easier to understand. The present invention can be embodied in many different forms of embodiments, and the protection scope of the present invention is not limited to the embodiments mentioned herein. In this application, k-space is cylindrical space. The z-direction in the cylindrical k-space is the central axis direction, also called the kz-direction or the layer-selective coding direction.
本申请提供的一种基于三维非笛卡尔轨迹的多回波采样方法,用于定量磁化率成像技术中,具体包括:A multi-echo sampling method based on a three-dimensional non-Cartesian trajectory provided by this application is used in quantitative magnetic susceptibility imaging technology, and specifically includes:
步骤1、选定一个圆柱形k空间,根据定量磁化率成像扫描需求,定义k空间的大小。定义参数Nx、Ny、Nz作为圆柱形k空间x、y、z方向上的坐标最大值。当参数Nx、Ny、Nz被确定后,圆柱形k空间也被唯一地确定。其中,x-y平面为与圆柱形k空间的顶面、底面平行的平面,z轴为圆柱形k空间的中轴线。Step 1. Select a cylindrical k-space, and define the size of the k-space according to the quantitative magnetic susceptibility imaging scanning requirements. The parameters Nx, Ny, Nz are defined as the coordinate maxima in the x, y, z directions of the cylindrical k-space. When the parameters Nx, Ny, and Nz are determined, the cylindrical k-space is also uniquely determined. The x-y plane is a plane parallel to the top and bottom surfaces of the cylindrical k-space, and the z-axis is the central axis of the cylindrical k-space.
在确定大小的圆柱形k空间内,选取多个x-y平面作为采集平面。并对这些采集平面进行编码。定义第i次选层编码时的采集平面的z坐标为多个采集平面之间的间距可以是等间距的,也可以是非等间距的。In a cylindrical k-space of a certain size, multiple xy planes are selected as acquisition planes. And encode these acquisition planes. Define the z-coordinate of the acquisition plane during the i-th layer selection encoding as The distances between the multiple acquisition planes may be equidistant or non-equidistant.
例如,当采用等间距次序编码时,可采用如下关系式确定 For example, when equidistant order coding is used, the following relation can be used to determine
其中,为第i次选层编码时的采集平面的选层方向(即z方向)坐标,Nz为圆柱形k空间选层方向上坐标的最大值,i为正整数,i=1,2,...,Nz。in, is the coordinate of the layer selection direction (that is, the z direction) of the acquisition plane during the i-th layer selection encoding, N z is the maximum value of the coordinates in the layer selection direction of the cylindrical k-space, i is a positive integer, i=1,2,. ..,N z .
当采用非等间距次序编码时,可以优选采用如下黄金比例次序编码来确定 When using non-equidistant sequence coding, the following golden ratio sequence coding can be preferably used to determine
其中,γ为比例系数,mod()为取余运算,为第i次选层编码时的采集平面的选层方向坐标,Nz为圆柱形k空间选层方向上坐标的最大值,i为正整数,i=1,2,...,Nz。Among them, γ is the proportional coefficient, mod() is the remainder operation, is the layer selection direction coordinates of the acquisition plane during the i-th layer selection encoding, N z is the maximum value of the coordinates in the cylindrical k-space layer selection direction, i is a positive integer, i=1,2,...,N z .
对于黄金比例次序编码,γ优选为黄金比例数,即:For golden ratio sequential coding, γ is preferably the golden ratio number, that is:
在其他类似的实施例中,选层编码次序还可以采用随机编码等次序。In other similar embodiments, the layer selection coding sequence may also adopt an sequence such as random coding.
步骤2、在步骤1中选取的等间距或非等间距的采集平面中,构建采集曲线。如图1所示为本实施例中优选的采集曲线。该采集曲线为呈玫瑰花瓣的螺旋状轨迹。其特点在于,采集坐标可以周期性地回到采集平面的中心原点,以此实现多回波数据采集。图1中所示的采集曲线为五个花瓣,即可以提供五个回波信号。在其他类似的实施例中,可以通过以下关系来设置采集曲线,并通过参数调整来决定花瓣的数量:Step 2. In the equidistant or non-equidistant acquisition planes selected in step 1, construct an acquisition curve. Figure 1 shows the preferred acquisition curve in this embodiment. The acquisition curve is a spiral trajectory in the form of rose petals. Its characteristic is that the acquisition coordinates can periodically return to the center origin of the acquisition plane, so as to realize multi-echo data acquisition. The acquisition curve shown in Figure 1 has five petals, that is, five echo signals can be provided. In other similar embodiments, the acquisition curve can be set through the following relationship, and the number of petals can be determined through parameter adjustment:
kx(t)=Nx·sin(ω1t)·cos(ω2t)k x (t)=N x ·sin(ω 1 t) ·cos(ω 2 t)
ky(t)=Ny·sin(ω1t)·sin(ω2t)k y (t)=N y ·sin(ω 1 t) ·sin(ω 2 t)
其中,kx、ky分别为x、y方向上的坐标;Nx、Ny分别是圆柱形k空间x、Among them, k x and ky are the coordinates in the x and y directions, respectively; N x and N y are the cylindrical k-space x,
y方向上的坐标最大值;ω1与ω2表示kx与ky的向采集曲线的振荡频率。通过调整ω1与ω2可以具体改变采集曲线花瓣的数量。The maximum value of the coordinates in the y direction; ω 1 and ω 2 represent the oscillation frequencies of the acquisition curves of k x and k y . By adjusting ω 1 and ω 2 , the number of petals in the collection curve can be specifically changed.
步骤3、根据多个采集平面的编码以及每一个采集曲线确定三维非笛卡尔轨迹。如图2所示为本实施例构建的三维非笛卡尔采集轨迹。在圆柱形k空间20中,等间距地选取了三个采集平面,并在各个采集平面上设置了五花瓣的采集曲线21、22、23。Step 3: Determine a three-dimensional non-Cartesian trajectory according to the codes of the multiple acquisition planes and each acquisition curve. FIG. 2 shows the three-dimensional non-Cartesian acquisition trajectory constructed in this embodiment. In the cylindrical k-
步骤4、根据三维非笛卡尔轨迹设计扫描时间序列。本实施例根据图3中选取的采集平面以及采集曲线,设计了如图3所示的基于三维非笛卡尔轨迹多回波采样序列。Step 4. Design the scanning time series according to the three-dimensional non-Cartesian trajectory. In this embodiment, according to the acquisition plane and acquisition curve selected in FIG. 3 , a multi-echo sampling sequence based on a three-dimensional non-Cartesian trajectory as shown in FIG. 3 is designed.
图3中,RF为射频激发脉冲,Gx为x轴施加的磁场梯度,Gy为y轴施加的磁场梯度,Gz为z轴施加的磁场梯度。其中z轴为选层编码方向。300为射频(Radiofrequency,RF)激发脉冲;301与302构成选层梯度;303为选层方向编码梯度;304与305为读出编码梯度;306,307,308分别表示三个编码方向的破坏梯度;309为下一个RF激发脉冲;310表示第一个回波信号时间,311表示第二个回波信号时间,312表示第三个回波信号时间,313表示第四个回波信号时间,314表示第五个回波信号时间,315表示扫描时间序列的重复时间。In Fig. 3, RF is the radio frequency excitation pulse, Gx is the magnetic field gradient applied on the x-axis, Gy is the magnetic field gradient applied on the y-axis, and Gz is the magnetic field gradient applied on the z-axis. The z-axis is the encoding direction of the selected layer. 300 is the radio frequency (Radiofrequency, RF) excitation pulse; 301 and 302 constitute the layer selection gradient; 303 is the layer selection direction encoding gradient; 304 and 305 are the readout encoding gradient; ; 309 is the next RF excitation pulse; 310 is the first echo signal time, 311 is the second echo signal time, 312 is the third echo signal time, 313 is the fourth echo signal time, 314 Denotes the fifth echo signal time, and 315 denotes the repetition time of the scan time series.
步骤5、根据上述设计的扫描时间序列,实施共振数据采集。Step 5, according to the scanning time sequence designed above, implement resonance data acquisition.
以上详细描述了本发明的较佳具体实施例。应当理解,本领域的普通技术无需创造性劳动就可以根据本发明的构思作出诸多修改和变化。因此,凡本技术领域中技术人员依本发明的构思在现有技术的基础上通过逻辑分析、推理或者有限的试验可以得到的技术方案,皆应在由权利要求书所确定的保护范围内。The preferred embodiments of the present invention have been described in detail above. It should be understood that many modifications and changes can be made according to the concept of the present invention by those skilled in the art without creative efforts. Therefore, any technical solutions that can be obtained by those skilled in the art through logical analysis, reasoning or limited tests on the basis of the prior art according to the concept of the present invention shall fall within the protection scope determined by the claims.
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Citations (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6404194B1 (en) * | 1994-08-05 | 2002-06-11 | The Board Of Trustees Of The Leland Stanford Junior University | Three dimensional magnetic resonance imaging using spiral trajectories in k-space |
CN1973211A (en) * | 2004-05-14 | 2007-05-30 | 皇家飞利浦电子股份有限公司 | Contrast prepared MRI involving non-cartesian trajectories with oversampling of the center of K-space |
CN106264529A (en) * | 2016-11-04 | 2017-01-04 | 深圳先进技术研究院 | Cylindrical k-space acquisition method and system for Three-Dimensional Dynamic nuclear magnetic resonance |
CN106264530A (en) * | 2016-11-04 | 2017-01-04 | 深圳先进技术研究院 | Cartesian k-space acquisition method and system for Three-Dimensional Dynamic nuclear magnetic resonance |
CN107750338A (en) * | 2015-06-15 | 2018-03-02 | 皇家飞利浦有限公司 | The MR gathered using star lamination is imaged |
CN110109036A (en) * | 2019-05-24 | 2019-08-09 | 厦门大学 | Two-dimension time-space coding sweeps the sampling of magnetic resonance imaging non-Cartesian and method for reconstructing |
CN110389310A (en) * | 2018-04-16 | 2019-10-29 | 西门子医疗有限公司 | Method and control device for producing magnetic resonance recordings |
EP3702799A1 (en) * | 2019-03-01 | 2020-09-02 | Canon Medical Systems Corporation | Mri apparatus and mri method |
Family Cites Families (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US8456163B2 (en) * | 2009-07-10 | 2013-06-04 | Siemens Medical Solutions Usa, Inc. | Variable image resolution MR imaging system |
US9465091B2 (en) * | 2010-01-04 | 2016-10-11 | Mayo Foundation For Medical Education And Research | System and method for random cartesian acquisition with projection reconstruction-like sampling |
US10429469B2 (en) * | 2012-04-11 | 2019-10-01 | Dignity Health | System and method for magnetic resonance imaging using three-dimensional, distributed, non-Cartesian sampling trajectories |
WO2013159044A1 (en) * | 2012-04-19 | 2013-10-24 | New York University | System, method and computer-accessible medium for highly-accelerated dynamic magnetic resonance imaging using golden-angle radial samplng and compressed sensing |
DE102015107347A1 (en) * | 2015-05-11 | 2016-11-17 | Universitätsspital Basel | A MAGNETIC RESONANCE TOMOGRAPHY PROCESS WITH ASYMMETRIC RADIAL ACQUISITION OF K-ROOM DATA |
US10281542B2 (en) * | 2015-09-30 | 2019-05-07 | General Electric Company | Magnetic resonance imaging system and method |
US10670684B2 (en) * | 2016-01-06 | 2020-06-02 | Siemens Healthcare Gmbh | Free-breathing non-contrast MR angiography |
DE102016224175B4 (en) * | 2016-12-06 | 2025-02-27 | Siemens Healthineers Ag | EPI with zigzag trajectory and parallel imaging |
US10466329B2 (en) * | 2017-04-06 | 2019-11-05 | Mayo Foundation For Medical Education And Research | Partial Fourier acquisition and reconstruction for k-space shells based magnetic resonance imaging |
US20190054194A1 (en) * | 2017-08-17 | 2019-02-21 | Case Western Reserve University | System and Method For Evaluation of Subjects Using Magnetic Resonance Imaging and Oxygen-17 |
US10996300B2 (en) * | 2018-09-05 | 2021-05-04 | Siemens Healthcare Gmbh | Cartesian-radial hybrid k-space trajectory for volumetric imaging |
-
2020
- 2020-11-26 CN CN202011347666.6A patent/CN112557978B/en active Active
Patent Citations (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6404194B1 (en) * | 1994-08-05 | 2002-06-11 | The Board Of Trustees Of The Leland Stanford Junior University | Three dimensional magnetic resonance imaging using spiral trajectories in k-space |
CN1973211A (en) * | 2004-05-14 | 2007-05-30 | 皇家飞利浦电子股份有限公司 | Contrast prepared MRI involving non-cartesian trajectories with oversampling of the center of K-space |
CN107750338A (en) * | 2015-06-15 | 2018-03-02 | 皇家飞利浦有限公司 | The MR gathered using star lamination is imaged |
CN106264529A (en) * | 2016-11-04 | 2017-01-04 | 深圳先进技术研究院 | Cylindrical k-space acquisition method and system for Three-Dimensional Dynamic nuclear magnetic resonance |
CN106264530A (en) * | 2016-11-04 | 2017-01-04 | 深圳先进技术研究院 | Cartesian k-space acquisition method and system for Three-Dimensional Dynamic nuclear magnetic resonance |
CN110389310A (en) * | 2018-04-16 | 2019-10-29 | 西门子医疗有限公司 | Method and control device for producing magnetic resonance recordings |
EP3702799A1 (en) * | 2019-03-01 | 2020-09-02 | Canon Medical Systems Corporation | Mri apparatus and mri method |
CN110109036A (en) * | 2019-05-24 | 2019-08-09 | 厦门大学 | Two-dimension time-space coding sweeps the sampling of magnetic resonance imaging non-Cartesian and method for reconstructing |
Non-Patent Citations (10)
Title |
---|
A fast & accurate non-iterative algorithm for regularized non-Cartesian MRI;Satyananda Kashyap;《2010 IEEE International Symposium on Biomedical Imaging: From Nano to Macro》;20100621;全文 * |
Data-driven MRSI spectral localization using non-cartesian sampling trajectories;Jeffrey Kasten;《2013 IEEE 10th International Symposium on Biomedical Imaging》;20130715;全文 * |
High Performance Non-uniform FFT on Modern X86-based Multi-core Systems;Dhiraj D. Kalamkar;《2012 IEEE 26th International Parallel and Distributed Processing Symposium》;20120816;全文 * |
Iterative image reconstruction in MRI with separate magnitude and phase regularization;J.A. Fessler;《2004 2nd IEEE International Symposium on Biomedical Imaging: Nano to Macro (IEEE Cat No. 04EX821)》;20050307;全文 * |
Iterative reconstruction of magnetic resonance images from arbitrary samples in k-space;B. Desplanques;《2001 IEEE Nuclear Science Symposium Conference Record (Cat. No.01CH37310)》;20020807;全文 * |
The iterative next-neighbor regridding (INNG) algorithm combined with TV regularization used for reconstruction in diffraction tomography;Tingting Li;《 2010 International Conference on Bioinformatics and Biomedical Technology》;20100603;全文 * |
Variable-FOV Reconstruction for 3D Non-Cartesian Parallel Imaging;Celal Furkan Senel;《 2017 21st National Biomedical Engineering Meeting (BIYOMUT)》;20181004;全文 * |
动态磁共振成像中利用时空滤波的非笛卡尔稀疏数据重建新算法;梅颖洁;《北京生物医学工程》;20110831;全文 * |
快速回波平面磁共振谱成像数据重建算法;黄敏;《生物医学工程学杂志》;20051231;全文 * |
非笛卡尔并行磁共振成像数据的自适应约束重建新算法;周爱珍;《中国生物医学工程学报》;20110430;全文 * |
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