CN115778353B - Magnetic field free line magnetic particle imaging method based on rotation harmonic diagram - Google Patents

Magnetic field free line magnetic particle imaging method based on rotation harmonic diagram Download PDF

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CN115778353B
CN115778353B CN202310054783.0A CN202310054783A CN115778353B CN 115778353 B CN115778353 B CN 115778353B CN 202310054783 A CN202310054783 A CN 202310054783A CN 115778353 B CN115778353 B CN 115778353B
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田捷
李光辉
刘晏君
安羽
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Beihang University
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Abstract

The invention belongs to the technical field of magnetic particle imaging, in particular relates to a magnetic field free line magnetic particle imaging method, a magnetic field free line magnetic particle imaging system and magnetic field free line magnetic particle imaging equipment based on a rotation harmonic diagram, and aims to solve the problems that a measuring process of a system matrix of the existing magnetic particle imaging method is complex, time consuming, large in occupied memory and long in calculation time, system correction efficiency of the magnetic particle imaging equipment is severely limited, and imaging instantaneity is low. The method comprises the following steps: setting related parameters of a magnetic particle imaging device based on a magnetic field free line, and starting and operating the magnetic particle imaging device; constructing system function harmonic graphs of different orders; measuring response signals of a target object to be imaged under each rotation angle and constructing an observation vector sequence; rotating the system function harmonic graphs of different orders to construct a system matrix under each rotation angle; reconstructing a magnetic particle image. The invention constructs the system matrix with other rotation angles by rotating the harmonic diagram, greatly reduces the complexity of system matrix measurement and improves the system correction efficiency of the magnetic particle imaging equipment.

Description

基于旋转谐波图的磁场自由线磁粒子成像方法Free-line Magnetic Particle Imaging Method Based on Rotational Harmonic Map

技术领域technical field

本发明属于磁粒子成像技术领域,具体涉及一种基于旋转谐波图的磁场自由线磁粒子成像方法、系统、设备。The invention belongs to the technical field of magnetic particle imaging, and in particular relates to a magnetic particle imaging method, system and equipment based on a rotating harmonic diagram of a magnetic field free line.

背景技术Background technique

近年来,活体无创分子影像技术快速发展,实现了对多种生物分子的在体有效观测。磁粒子成像技术基于磁纳米粒子的非线性磁化响应进行成像,具有高灵敏度、高空间分辨率、无辐射、无背景信号干扰和无成像深度限制等优势,有望应用于深层微小肿瘤检测、心脑血管功能监测等重大临床问题。In recent years, the rapid development of in vivo non-invasive molecular imaging technology has realized the effective observation of various biomolecules in vivo. Magnetic particle imaging technology is based on the nonlinear magnetization response of magnetic nanoparticles for imaging. It has the advantages of high sensitivity, high spatial resolution, no radiation, no background signal interference, and no limitation of imaging depth. It is expected to be applied to deep micro-tumor detection, heart and brain Major clinical issues such as vascular function monitoring.

磁粒子成像技术使用磁场组合来探测磁纳米粒子示踪剂的浓度分布情况,其中磁场包括静态和动态磁场。静态磁场为不均匀恒定磁场,或称为梯度磁场,其突出特征为包含一个或多个低磁场区域,形状通常为椭圆形点状的磁场自由点或直线型的磁场自由线。磁纳米粒子在低强度磁场区域内为非饱和状态,在外加磁场激励时产生信号,并被接收线圈探测;但在高强度磁场区域内为饱和状态,被激励后信号微弱,无法被探测到。动态场为均匀交变磁场,或称为激励磁场,用于驱动低磁场区域在成像视野内移动和激励磁纳米粒子产生非线性特征信号。磁粒子成像使用激励磁场驱动低磁场区域在成像视野内扫描特定轨迹,完成磁纳米粒子浓度的空间编码。相比于磁场自由点,磁场自由线的低磁场区域更大,单次扫描覆盖的范围更大,信噪比更高而且成像速度更快,在近年来已得到广泛研究和应用。Magnetic particle imaging uses a combination of magnetic fields, both static and dynamic, to probe the concentration distribution of magnetic nanoparticle tracers. The static magnetic field is an inhomogeneous constant magnetic field, or called a gradient magnetic field. Its prominent feature is that it contains one or more low magnetic field regions, and its shape is usually an elliptical point-shaped free point of the magnetic field or a linear free line of the magnetic field. Magnetic nanoparticles are in a non-saturated state in the low-intensity magnetic field region, and generate signals when excited by an external magnetic field, and are detected by the receiving coil; but in a saturated state in the high-intensity magnetic field region, the signal is weak after being excited and cannot be detected. The dynamic field is a uniform alternating magnetic field, or called an excitation magnetic field, which is used to drive the low magnetic field region to move within the imaging field of view and to excite magnetic nanoparticles to generate nonlinear characteristic signals. Magnetic particle imaging uses an excitation magnetic field to drive a low magnetic field region to scan a specific trajectory within the imaging field of view to complete the spatial encoding of the concentration of magnetic nanoparticles. Compared with the magnetic field free point, the low magnetic field area of the magnetic field free line is larger, the single scan covers a larger area, the signal-to-noise ratio is higher, and the imaging speed is faster. It has been widely studied and applied in recent years.

从信号到图像的重建过程是磁粒子成像的重要步骤,其中一种重要的方法是系统矩阵法。目前,系统矩阵法的步骤为:测量单位样本在成像视野中每一个像素点处的信号频谱,筛选后在频域内构建表征成像系统的系统矩阵,将被测物体的信号量化为观测向量,建立线性方程组,通过求解线性方程组的方式来重建。基于磁场自由线的磁粒子成像系统,需要旋转磁场自由线或者旋转被测物体,覆盖全部成像视野后才能准确重建。所以传统方法中,每旋转一定角度的磁场自由线或被测物体,就需要测量一次系统矩阵。这个过程复杂、耗时,占用内存大,计算时间长,严重限制了磁粒子成像设备的系统校正效率,难以实时成像,所以需要一种更加高效的基于系统矩阵的磁场自由线磁粒子成像方法。The reconstruction process from signal to image is an important step in magnetic particle imaging, and one of the important methods is the system matrix method. At present, the steps of the system matrix method are: measure the signal spectrum of the unit sample at each pixel in the imaging field of view, construct a system matrix representing the imaging system in the frequency domain after screening, quantify the signal of the measured object into an observation vector, and establish A system of linear equations, reconstructed by solving a system of linear equations. The magnetic particle imaging system based on the free line of the magnetic field needs to rotate the free line of the magnetic field or the measured object to cover the entire imaging field of view before accurate reconstruction can be performed. Therefore, in the traditional method, the system matrix needs to be measured once every time the free line of the magnetic field or the measured object is rotated at a certain angle. This process is complex, time-consuming, takes up a lot of memory, and takes a long time to calculate, which severely limits the system calibration efficiency of magnetic particle imaging equipment, and it is difficult to perform real-time imaging. Therefore, a more efficient magnetic particle imaging method based on system matrix free lines of magnetic field is needed.

传统方法中测量所有角度下的系统矩阵的原因在于:经旋转后,磁场出现轻微的扭曲或变形。所以测量每个旋转角度下的系统矩阵,是对成像系统最准确的测量和建模方法。但在旋转过程中,不同角度间的系统矩阵存在高度的信息相似性。The reason for measuring the system matrix at all angles in the traditional method is that after rotation, the magnetic field is slightly distorted or deformed. Therefore, measuring the system matrix at each rotation angle is the most accurate measurement and modeling method for the imaging system. However, during the rotation process, there is a high degree of information similarity in the system matrix between different angles.

分析磁粒子成像过程,系统矩阵表达了在成像视野内每个像素处的各阶谐波响应,谐波图反映了系统本身的空间响应频率。对于旋转磁场自由线,通过控制通电参数或机械旋转梯度线圈使得成像系统本身发生旋转,可以认为系统矩阵中的谐波图也随之旋转,但稍有变形;对于旋转被测物体,系统本身并未发生改变,但通过转换坐标系也反映了同样的旋转过程。所以传统方法中,不同角度间的系统矩阵必然存在高度重复性信息。基于此,本发明提出了一种基于旋转谐波图的磁场自由线磁粒子成像方法。Analyzing the magnetic particle imaging process, the system matrix expresses the harmonic response of each order at each pixel in the imaging field of view, and the harmonic map reflects the spatial response frequency of the system itself. For the free line of the rotating magnetic field, the imaging system itself is rotated by controlling the electrification parameters or mechanically rotating the gradient coil, and it can be considered that the harmonic diagram in the system matrix also rotates with it, but with a slight deformation; for the rotating measured object, the system itself does not Unchanged, but the same rotation is reflected by transforming the coordinate system. Therefore, in the traditional method, there must be highly repetitive information in the system matrix between different angles. Based on this, the present invention proposes a method for magnetic particle imaging of free lines of magnetic field based on rotation harmonic diagram.

发明内容Contents of the invention

为了解决现有技术中的上述问题,即为了解决现有基于系统矩阵的磁粒子成像方法每旋转一定角度的磁场自由线或被测物体,就需要测量一次系统矩阵,测量过程复杂、耗时,占用内存大,计算时间长,严重限制了磁粒子成像设备的系统校正效率,成像实时性较低的问题,本发明提出了一种基于旋转谐波图的磁场自由线磁粒子成像方法,应用于基于磁场自由线的磁粒子成像装置,该方法包括:In order to solve the above problems in the prior art, that is, in order to solve the existing magnetic particle imaging method based on the system matrix, the system matrix needs to be measured once every time the free magnetic field line or the measured object is rotated at a certain angle, and the measurement process is complicated and time-consuming. It takes up a lot of memory and takes a long time to calculate, which seriously limits the system correction efficiency of magnetic particle imaging equipment, and the real-time performance of imaging is low. A magnetic particle imaging device based on free lines of a magnetic field, the method comprising:

步骤S100,设置所述基于磁场自由线的磁粒子成像装置的相关参数,开启并运行所述基于磁场自由线的磁粒子成像装置;所述相关参数包括成像视野半径大小、选择磁场梯度、激励磁场幅值与频率、数字采样频率与时间、单位样本大小;Step S100, setting the relevant parameters of the magnetic particle imaging device based on free lines of magnetic field, starting and running the magnetic particle imaging device based on free lines of magnetic field; the relevant parameters include imaging field of view radius, selected magnetic field gradient, excitation magnetic field Amplitude and frequency, digital sampling frequency and time, unit sample size;

步骤S200,设置所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置的位置与方向,并结合所述成像视野半径,设置单位样本的移动路径;按照设定的移动路径移动单位样本,测量所述基于磁场自由线的磁粒子成像装置成像视野范围内每一个像素处单位样本的信号,进而构建不同阶的系统函数谐波图;所述系统矩阵测量装置为根据设定移动路径将单位样本移动至指定位置的装置;Step S200, setting the position and direction of the system matrix measuring device in the magnetic particle imaging device based on free lines of magnetic field, and combining the imaging field of view radius, setting the moving path of the unit sample; moving the unit sample according to the set moving path, Measure the signal of the unit sample at each pixel within the imaging field of view of the magnetic particle imaging device based on the free lines of the magnetic field, and then construct system function harmonic diagrams of different orders; A device for moving samples to designated locations;

步骤S300,以所述系统矩阵测量装置的方向为初始方向,设置旋转角度以及旋转顺序;按照所述旋转角度及所述旋转顺序旋转所述基于磁场自由线的磁粒子成像装置的磁场自由线或者待成像的目标对象,测量各旋转角度下待成像的目标对象的响应信号并构建观测向量序列;Step S300, taking the direction of the system matrix measuring device as the initial direction, setting the rotation angle and the rotation sequence; rotating the magnetic field free lines of the magnetic particle imaging device based on the magnetic field free lines or The target object to be imaged, measuring the response signal of the target object to be imaged at each rotation angle and constructing an observation vector sequence;

步骤S400,按照所述旋转角度,旋转不同阶的系统函数谐波图,并基于旋转后的不同阶的系统函数谐波图构建各旋转角度下的系统矩阵;Step S400, according to the rotation angle, rotate the harmonic diagram of the system function of different orders, and construct the system matrix under each rotation angle based on the rotated harmonic diagram of the system function of different orders;

步骤S500,将所述观测向量序列按列进行合并、将各旋转角度下的系统矩阵按列进行合并,合并后,构建线性方程组;对所述线性方程组求解,得到待成像的目标对象对应重建的磁粒子图像。Step S500, combining the observation vector sequence by column, merging the system matrices under each rotation angle by column, and constructing a linear equation system after merging; solving the linear equation system to obtain the corresponding Reconstructed magnetic particle image.

在一些优选的实施方式中,测量每一个像素出单位样本的信号,进而构建不同阶的系统函数谐波图,其方法为:In some preferred embodiments, the signal of each pixel out of the unit sample is measured, and then the harmonic diagram of the system function of different orders is constructed, and the method is as follows:

测量每一个像素处单位样本的时域信号,并通过快速傅里叶变换得到频谱;Measure the time-domain signal of the unit sample at each pixel, and obtain the frequency spectrum through fast Fourier transform;

根据所述基于磁场自由线的磁粒子成像装置的信噪比,筛选信噪比大于设定信噪比阈值的谐波信号,将筛选后的谐波信号作为第一谐波信号;基于所述频谱,将各像素处相同阶的第一谐波信号进行合成,得到不同阶的系统函数谐波图。According to the signal-to-noise ratio of the magnetic particle imaging device based on the free line of magnetic field, filter the harmonic signal whose signal-to-noise ratio is greater than the set signal-to-noise ratio threshold, and use the filtered harmonic signal as the first harmonic signal; based on the said Spectrum, the first harmonic signals of the same order at each pixel are synthesized to obtain system function harmonic diagrams of different orders.

在一些优选的实施方式中,设置旋转角度以及旋转顺序,其方法为:In some preferred implementations, the rotation angle and rotation sequence are set, and the method is as follows:

以所述初始方向为0°,按照等间距或不等间距方式步进旋转至180°,保证磁场自由线的运动范围能够覆盖全部成像视野,共旋转N个角度;其中,N表示设定数量。Taking the initial direction as 0°, stepping and rotating to 180° according to equal intervals or unequal intervals, ensuring that the range of motion of the free line of the magnetic field can cover the entire imaging field of view, and rotate N angles in total; where N represents the set number .

在一些优选的实施方式中,测量各旋转角度下待成像的目标对象的响应信号并构建观测向量序列,其方法为:In some preferred embodiments, the response signal of the target object to be imaged at each rotation angle is measured and the observation vector sequence is constructed, the method is:

测量各旋转角度下待成像的目标对象的响应信号并构建当前旋转角度下的观测列向量,进而构建所有旋转角度下的观测向量序列;Measure the response signal of the target object to be imaged at each rotation angle and construct the observation column vector at the current rotation angle, and then construct the observation vector sequence at all rotation angles;

所述观测列向量为根据所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置初始方向下的系统矩阵使用的特征谐波提取对应旋转角度下待成像的目标物体的响应信号的特征谐波构建的列向量。The observation column vector is the characteristic harmonic used to extract the response signal of the target object to be imaged at the corresponding rotation angle according to the characteristic harmonic used by the system matrix in the initial direction of the system matrix measuring device in the magnetic particle imaging device based on free lines of magnetic field Column vector of wave builds.

在一些优选的实施方式中,在旋转不同阶的系统函数谐波图时分解为实部谐波图、虚部谐波图,旋转后合成为复数谐波图;In some preferred embodiments, when rotating the harmonic diagram of the system function of different orders, it is decomposed into a real part harmonic diagram and an imaginary part harmonic diagram, and synthesized into a complex harmonic diagram after rotation;

旋转不同阶的系统函数谐波图后保持图像大小不变,无像素点处使用零填充,非网格像素点处使用插值方法取整。Keep the size of the image unchanged after rotating the harmonic diagram of the system function of different orders, use zero padding at the non-grid pixel points, and use the interpolation method to round the non-grid pixel points.

在一些优选的实施方式中,构建线性方程组,其方法为:In some preferred embodiments, construct linear equation system, its method is:

  ; ; ;

其中,表示各旋转角度下的系统矩阵{A1,A2, ..., AN}按列进行合并系统矩阵,表示所述观测向量序列{b1, b2, ..., bN}中所有观测向量按列合并后的观测向量,表示待成像的目标物体的离散向量形式。in, Represents the system matrix {A 1, A 2 , ..., A N } at each rotation angle to merge the system matrix by column, Represents the observation vector after all the observation vectors in the observation vector sequence {b 1 , b 2 , ..., b N } are merged by columns, A discrete vector form representing the target object to be imaged.

本发明的第二方面,提出了一种基于旋转谐波图的磁场自由线磁粒子成像系统,该系统包括:初始化设置模块、谐波图构建模块、观测向量构建模块、系统矩阵构建模块、图像重建模块;In the second aspect of the present invention, a magnetic field free-line magnetic particle imaging system based on a rotating harmonic diagram is proposed. The system includes: an initialization setting module, a harmonic diagram building module, an observation vector building module, a system matrix building module, an image rebuild module;

所述初始化设置模块,配置为设置所述基于磁场自由线的磁粒子成像装置的相关参数,开启并运行所述基于磁场自由线的磁粒子成像装置;所述相关参数包括成像视野半径大小、选择磁场梯度、激励磁场幅值与频率、数字采样频率与时间、单位样本大小;The initialization setting module is configured to set the relevant parameters of the magnetic particle imaging device based on free lines of magnetic field, start and run the magnetic particle imaging device based on free lines of magnetic field; the relevant parameters include imaging field of view radius, selection Magnetic field gradient, excitation magnetic field amplitude and frequency, digital sampling frequency and time, unit sample size;

所述谐波图构建模块,配置为设置所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置的位置与方向,并结合所述成像视野半径,设置单位样本的移动路径;按照设定的移动路径移动单位样本,测量所述基于磁场自由线的磁粒子成像装置成像视野范围内每一个像素处单位样本的信号,进而构建不同阶的系统函数谐波图;所述系统矩阵测量装置为根据设定移动路径将单位样本移动至指定位置的装置;The harmonic diagram construction module is configured to set the position and direction of the system matrix measurement device in the magnetic particle imaging device based on free lines of magnetic field, and combine the imaging field of view radius to set the moving path of the unit sample; according to the setting Move the unit sample according to the moving path, measure the signal of the unit sample at each pixel within the imaging field of view of the magnetic particle imaging device based on the free line of magnetic field, and then construct the harmonic diagram of the system function of different orders; the system matrix measurement device is A device that moves a unit sample to a designated location according to a set movement path;

所述观测向量构建模块,配置为以所述系统矩阵测量装置的方向为初始方向,设置旋转角度以及旋转顺序;按照所述旋转角度及所述旋转顺序旋转所述基于磁场自由线的磁粒子成像装置的磁场自由线或者待成像的目标对象,测量各旋转角度下待成像的目标对象的响应信号并构建观测向量序列;The observation vector construction module is configured to take the direction of the system matrix measurement device as the initial direction, set the rotation angle and the rotation sequence; rotate the magnetic particle imaging based on the free line of the magnetic field according to the rotation angle and the rotation sequence The free line of the magnetic field of the device or the target object to be imaged, measuring the response signal of the target object to be imaged at each rotation angle and constructing an observation vector sequence;

所述系统矩阵构建模块,配置为按照所述旋转角度,旋转不同阶的系统函数谐波图,并基于旋转后的不同阶的系统函数谐波图构建各旋转角度下的系统矩阵;The system matrix construction module is configured to rotate the system function harmonic diagrams of different orders according to the rotation angle, and construct the system matrix at each rotation angle based on the rotated system function harmonic diagrams of different orders;

所述图像重建模块,配置为将所述观测向量序列按列进行合并、将各旋转角度下的系统矩阵按列进行合并,合并后,构建线性方程组;对所述线性方程组求解,得到待成像的目标对象对应重建的磁粒子图像。The image reconstruction module is configured to combine the observation vector sequence by column, and combine the system matrices under each rotation angle by column. After the combination, construct a linear equation system; solve the linear equation system to obtain The imaged target object corresponds to the reconstructed magnetic particle image.

本发明的第三方面,提出了一种电子设备,包括:至少一个处理器;以及与至少一个所述处理器通信连接的存储器;其中,所述存储器存储有可被所述处理器执行的指令,所述指令用于被所述处理器执行以实现上述的基于旋转谐波图的磁场自由线磁粒子成像方法。In a third aspect of the present invention, an electronic device is proposed, including: at least one processor; and a memory connected to at least one processor in communication; wherein, the memory stores instructions executable by the processor , the instructions are used to be executed by the processor to implement the above method for magnetic particle imaging of free lines of magnetic field based on rotational harmonic diagrams.

本发明的第四方面,提出了一种计算机可读存储介质,所述计算机可读存储介质存储有计算机指令,所述计算机指令用于被所述计算机执行以实现上述的基于旋转谐波图的磁场自由线磁粒子成像方法。According to the fourth aspect of the present invention, a computer-readable storage medium is proposed, the computer-readable storage medium stores computer instructions, and the computer instructions are used to be executed by the computer to realize the above-mentioned rotating harmonic diagram-based Magnetic field free-line magnetic particle imaging method.

本发明的有益效果:Beneficial effects of the present invention:

本发明提出仅测量一个角度下的系统矩阵,通过旋转谐波图的方式来构建其他旋转角度的系统矩阵,进而完成全部系统矩阵的构建。这种方法将大大降低系统矩阵测量的复杂度,同时降低内存资源需求,提高磁粒子成像设备系统校正效率,提高了磁粒子成像的实时性。The present invention proposes to measure the system matrix at only one angle, and construct the system matrix of other rotation angles by rotating the harmonic diagram, and then complete the construction of all system matrices. This method will greatly reduce the complexity of system matrix measurement, reduce memory resource requirements, improve the system calibration efficiency of magnetic particle imaging equipment, and improve the real-time performance of magnetic particle imaging.

附图说明Description of drawings

通过阅读参照以下附图所做的对非限制性实施例所做的详细描述,本申请的其他特征、目的和优点将会变得更明显。Other features, objects and advantages of the present application will become more apparent by reading the detailed description of non-limiting embodiments made with reference to the following drawings.

图1 是本发明一种实施例的基于旋转谐波图的磁场自由线磁粒子成像方法的流程示意图;Fig. 1 is a schematic flow chart of a method for magnetic particle imaging of free lines of magnetic field based on a rotating harmonic diagram according to an embodiment of the present invention;

图2为本发明一种实施例的基于旋转谐波图的磁场自由线磁粒子成像方法的框架示意图;FIG. 2 is a schematic framework diagram of a magnetic particle imaging method based on a rotating harmonic diagram of a magnetic field free line according to an embodiment of the present invention;

图3是本发明一种实施例的旋转磁粒子成像装置的磁场自由线或者待成像的目标对象的示意图;Fig. 3 is a schematic diagram of the free lines of the magnetic field or the target object to be imaged in the rotating magnetic particle imaging device according to an embodiment of the present invention;

图4是本发明一种实施例的传统方法与本发明方法构建系统矩阵的过程示意图;Fig. 4 is a schematic diagram of the process of constructing a system matrix in a traditional method of an embodiment of the present invention and the method of the present invention;

图5是本发明一种实施例的旋转二次、三次、四次系统函数谐波图的示例图;Fig. 5 is an example diagram of the harmonic diagram of the second, third and fourth system functions of rotation in an embodiment of the present invention;

图6是本发明一种实施例的标准仿体与目标对象重建后的磁粒子图像的示意图;Fig. 6 is a schematic diagram of a standard phantom and a reconstructed magnetic particle image of a target object according to an embodiment of the present invention;

图7是本发明一种实施例的适于用来实现本申请实施例的电子设备的计算机系统的结构示意图。Fig. 7 is a schematic structural diagram of a computer system suitable for realizing the electronic device of the embodiment of the present application according to an embodiment of the present invention.

具体实施方式Detailed ways

为使本发明实施例的目的、技术方案和优点更加清楚,下面将结合本发明实施例中的附图,对本发明实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。In order to make the purpose, technical solutions and advantages of the embodiments of the present invention clearer, the technical solutions in the embodiments of the present invention will be clearly and completely described below in conjunction with the drawings in the embodiments of the present invention. Obviously, the described embodiments It is a part of embodiments of the present invention, but not all embodiments. Based on the embodiments of the present invention, all other embodiments obtained by persons of ordinary skill in the art without making creative efforts belong to the protection scope of the present invention.

下面结合附图和实施例对本申请作进一步的详细说明。可以理解的是,此处所描述的具体实施例仅仅用于解释相关发明,而非对该发明的限定。需要说明的是,在不冲突的情况下,本申请中的实施例及实施例中的特征可以相互组合。The application will be further described in detail below in conjunction with the accompanying drawings and embodiments. It should be understood that the specific embodiments described here are only used to explain related inventions, rather than to limit the invention. It should be noted that, in the case of no conflict, the embodiments in the present application and the features in the embodiments can be combined with each other.

本发明第一实施例的一种基于旋转谐波图的磁场自由线磁粒子成像方法,应用于基于磁场自由线的磁粒子成像装置;如图1所示,该方法包括:A method of magnetic particle imaging based on free lines of magnetic field based on rotational harmonic diagrams in the first embodiment of the present invention is applied to a magnetic particle imaging device based on free lines of magnetic field; as shown in FIG. 1 , the method includes:

步骤S100,设置所述基于磁场自由线的磁粒子成像装置的相关参数,开启并运行所述基于磁场自由线的磁粒子成像装置;所述相关参数包括成像视野半径大小、选择磁场梯度、激励磁场幅值与频率、数字采样频率与时间、单位样本大小;Step S100, setting the relevant parameters of the magnetic particle imaging device based on free lines of magnetic field, starting and running the magnetic particle imaging device based on free lines of magnetic field; the relevant parameters include imaging field of view radius, selected magnetic field gradient, excitation magnetic field Amplitude and frequency, digital sampling frequency and time, unit sample size;

步骤S200,设置所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置的位置与方向,并结合所述成像视野半径,设置单位样本的移动路径;按照设定的移动路径移动单位样本,测量所述基于磁场自由线的磁粒子成像装置成像视野范围内每一个像素处单位样本的信号,进而构建不同阶的系统函数谐波图;所述系统矩阵测量装置为根据设定移动路径将单位样本移动至指定位置的装置;Step S200, setting the position and direction of the system matrix measuring device in the magnetic particle imaging device based on free lines of magnetic field, and combining the imaging field of view radius, setting the moving path of the unit sample; moving the unit sample according to the set moving path, Measure the signal of the unit sample at each pixel within the imaging field of view of the magnetic particle imaging device based on the free lines of the magnetic field, and then construct system function harmonic diagrams of different orders; A device for moving samples to designated locations;

步骤S300,以所述系统矩阵测量装置的方向为初始方向,设置旋转角度以及旋转顺序;按照所述旋转角度及所述旋转顺序旋转所述基于磁场自由线的磁粒子成像装置的磁场自由线或者待成像的目标对象,测量各旋转角度下待成像的目标对象的响应信号并构建观测向量序列;Step S300, taking the direction of the system matrix measuring device as the initial direction, setting the rotation angle and the rotation sequence; rotating the magnetic field free lines of the magnetic particle imaging device based on the magnetic field free lines or The target object to be imaged, measuring the response signal of the target object to be imaged at each rotation angle and constructing an observation vector sequence;

步骤S400,按照所述旋转角度,旋转不同阶的系统函数谐波图,并基于旋转后的不同阶的系统函数谐波图构建各旋转角度下的系统矩阵;Step S400, according to the rotation angle, rotate the harmonic diagram of the system function of different orders, and construct the system matrix under each rotation angle based on the rotated harmonic diagram of the system function of different orders;

步骤S500,将所述观测向量序列按列进行合并、将各旋转角度下的系统矩阵按列进行合并,合并后,构建线性方程组;对所述线性方程组求解,得到待成像的目标对象对应重建的磁粒子图像。Step S500, combining the observation vector sequence by column, merging the system matrices under each rotation angle by column, and constructing a linear equation system after merging; solving the linear equation system to obtain the corresponding Reconstructed magnetic particle image.

为了更清晰地对本发明一种基于旋转谐波图的磁场自由线磁粒子成像方法进行说明,下面结合附图,对本发明方法一种实施例中各步骤进行展开详述。In order to more clearly describe a magnetic particle imaging method for free lines of magnetic field based on rotational harmonic diagrams of the present invention, the steps in an embodiment of the method of the present invention will be described in detail below in conjunction with the accompanying drawings.

步骤S100,设置所述基于磁场自由线的磁粒子成像装置的相关参数,开启并运行所述基于磁场自由线的磁粒子成像装置;所述相关参数包括成像视野半径大小、选择磁场梯度、激励磁场幅值与频率、数字采样频率与时间、单位样本大小;Step S100, setting the relevant parameters of the magnetic particle imaging device based on free lines of magnetic field, starting and running the magnetic particle imaging device based on free lines of magnetic field; the relevant parameters include imaging field of view radius, selected magnetic field gradient, excitation magnetic field Amplitude and frequency, digital sampling frequency and time, unit sample size;

在本实施例中,先初始化基于磁场自由线的磁粒子成像装置的相关参数,相关参数包括成像视野半径大小、选择磁场梯度、激励磁场幅值与频率、数字采样频率与时间、单位样本大小。初始化后开启并运行基于磁场自由线的磁粒子成像装置。In this embodiment, the related parameters of the magnetic particle imaging device based on free lines of magnetic field are first initialized, and the related parameters include imaging field of view radius, selected magnetic field gradient, excitation magnetic field amplitude and frequency, digital sampling frequency and time, and unit sample size. After initialization, turn on and run the magnetic particle imaging device based on free lines of magnetic field.

步骤S200,设置所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置的位置与方向,并结合所述成像视野半径,设置单位样本的移动路径;按照设定的移动路径移动单位样本,测量所述基于磁场自由线的磁粒子成像装置成像视野范围内每一个像素处单位样本的信号,进而构建不同阶的系统函数谐波图;所述系统矩阵测量装置为根据设定移动路径将单位样本移动至指定位置的装置;Step S200, setting the position and direction of the system matrix measuring device in the magnetic particle imaging device based on free lines of magnetic field, and combining the imaging field of view radius, setting the moving path of the unit sample; moving the unit sample according to the set moving path, Measure the signal of the unit sample at each pixel within the imaging field of view of the magnetic particle imaging device based on the free lines of the magnetic field, and then construct system function harmonic diagrams of different orders; A device for moving samples to designated locations;

在本实施例中,系统矩阵测量装置优选设置为三轴位移台或机械臂,能够根据设定路径将单位样本(本发明优选使用的是点状样本(论文中称之为delta phantom,暂无标准的中文翻译(具体参考文献:Top C , Gungor A . Tomographic Field Free LineMagnetic ParticleImaging With an Open-Sided Scanner Configuration[J]. IEEEtransactions onmedical imaging, 2020, 39(12):4164-4173.))通常其形状为像素或体素的形状,腔内装有磁纳米粒子,内部为立方体粒子腔)移动至指定位置。In this embodiment, the system matrix measurement device is preferably set as a three-axis translation platform or a mechanical arm, which can move the unit sample (the present invention preferably uses a point sample (called delta phantom in the paper, not available yet) according to the set path. Standard Chinese translation (specific references: Top C , Gungor A . Tomographic Field Free LineMagnetic Particle Imaging With an Open-Sided Scanner Configuration[J]. IEEEtransactions on medical imaging, 2020, 39(12):4164-4173.)) Usually its The shape is the shape of a pixel or a voxel, the cavity is filled with magnetic nanoparticles, and the interior is a cubic particle cavity) to move to a specified position.

先设置所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置的位置与方向,并结合所述成像视野半径,设置单位样本的移动路径;然后测量该方向下(即系统矩阵测量装置的初始方向)的系统矩阵A1作为系统基准,构建各阶系统函数谐波图;具体如下:First set the position and direction of the system matrix measurement device in the magnetic particle imaging device based on free lines of magnetic field, and combine the imaging field of view radius to set the moving path of the unit sample; then measure the direction (that is, the system matrix measurement device) The system matrix A 1 of the initial direction) is used as the system benchmark, and the harmonic diagram of the system function of each order is constructed; the details are as follows:

按照设定的移动路径移动单位样本,测量每一个像素处单位样本的时域信号,并通过快速傅里叶变换得到频谱;Move the unit sample according to the set moving path, measure the time-domain signal of the unit sample at each pixel, and obtain the spectrum through fast Fourier transform;

根据所述基于磁场自由线的磁粒子成像装置的信噪比,筛选信噪比大于设定信噪比阈值的谐波信号,将筛选后的谐波信号作为第一谐波信号;基于所述频谱,将各像素处相同阶的第一谐波信号进行合成,得到不同阶的系统函数谐波图。即系统函数谐波图为在当前磁粒子成像装置信噪比条件下能够探测到的所有粒子谐波信号,将所述基于磁场自由线的磁粒子成像装置成像视野内各像素或体素处的相同谐波合成为各阶系统函数谐波图,谐波信息为复数,谐波图可分解为实部谐波图和虚部谐波图;单位样本为在测试系统矩阵时使用的装有单位浓度磁纳米粒子的、与所述基于磁场自由线的磁粒子成像装置成像最高分辨率尺寸相同的载液腔体。According to the signal-to-noise ratio of the magnetic particle imaging device based on the free line of magnetic field, filter the harmonic signal whose signal-to-noise ratio is greater than the set signal-to-noise ratio threshold, and use the filtered harmonic signal as the first harmonic signal; based on the said Spectrum, the first harmonic signals of the same order at each pixel are synthesized to obtain system function harmonic diagrams of different orders. That is, the system function harmonic diagram is all the particle harmonic signals that can be detected under the condition of the signal-to-noise ratio of the current magnetic particle imaging device. The same harmonics are synthesized into harmonic diagrams of system functions of each order, and the harmonic information is complex numbers, and the harmonic diagrams can be decomposed into real part harmonic diagrams and imaginary part harmonic diagrams; the unit sample is the equipped unit used when testing the system matrix The liquid-carrying cavity with the same concentration of magnetic nanoparticles and the same size as the highest resolution imaging device of the magnetic particle imaging device based on free lines of magnetic field.

步骤S300,以所述系统矩阵测量装置的方向为初始方向,设置旋转角度以及旋转顺序;按照所述旋转角度及所述旋转顺序旋转所述基于磁场自由线的磁粒子成像装置的磁场自由线或者待成像的目标对象,测量各旋转角度下待成像的目标对象的响应信号并构建观测向量序列;Step S300, taking the direction of the system matrix measuring device as the initial direction, setting the rotation angle and the rotation sequence; rotating the magnetic field free lines of the magnetic particle imaging device based on the magnetic field free lines or The target object to be imaged, measuring the response signal of the target object to be imaged at each rotation angle and constructing an observation vector sequence;

在本实施例中,优选以所述初始方向为0°,按照等间距或不等间距方式步进旋转至180°,保证磁场自由线的运动范围能够覆盖全部成像视野(即旋转顺序的要求),共旋转N个角度;其中,N表示设定数量,在本实施例中,大于等于9,在其他实施例中,可以根据实际情况设置。In this embodiment, it is preferable to take the initial direction as 0°, and step and rotate to 180° according to equal or unequal intervals, so as to ensure that the range of motion of the free lines of the magnetic field can cover the entire imaging field of view (that is, the requirement of the rotation sequence) , a total of N angles are rotated; wherein, N represents the set number, in this embodiment, it is greater than or equal to 9, and in other embodiments, it can be set according to the actual situation.

按照所述旋转角度及所述旋转顺序旋转所述基于磁场自由线的磁粒子成像装置的磁场自由线或者待成像的目标对象,测量各旋转角度下待成像的目标对象的响应信号并构建观测向量序列,其方法为:Rotate the free lines of the magnetic field or the target object to be imaged of the magnetic particle imaging device based on the free line of magnetic field according to the rotation angle and the rotation sequence, measure the response signals of the target object to be imaged at each rotation angle and construct an observation vector sequence, its methods are:

按照所述旋转角度及所述旋转顺序旋转所述基于磁场自由线的磁粒子成像装置的磁场自由线或者待成像的目标对象,测量各旋转角度下待成像的目标对象的响应信号并构建当前旋转角度下的观测列向量,进而构建所有旋转角度下的观测向量序列;所述观测列向量为根据所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置初始方向下的系统矩阵使用的特征谐波提取对应旋转角度下待成像的目标物体的响应信号的特征谐波构建的列向量。Rotate the free lines of the magnetic field or the target object to be imaged of the magnetic particle imaging device based on the free line of magnetic field according to the rotation angle and the rotation sequence, measure the response signal of the target object to be imaged at each rotation angle and construct the current rotation The observation column vector under the angle, and then construct the observation vector sequence under all rotation angles; The observation column vector is the feature used according to the system matrix under the initial direction of the system matrix measurement device in the magnetic particle imaging device based on free lines of magnetic field The harmonic extraction is a column vector constructed by the characteristic harmonics of the response signal of the target object to be imaged corresponding to the rotation angle.

步骤S400,按照所述旋转角度,旋转不同阶的系统函数谐波图,并基于旋转后的不同阶的系统函数谐波图构建各旋转角度下的系统矩阵;Step S400, according to the rotation angle, rotate the harmonic diagram of the system function of different orders, and construct the system matrix under each rotation angle based on the rotated harmonic diagram of the system function of different orders;

在本实施例中,在旋转不同阶的系统函数谐波图时分解为实部谐波图、虚部谐波图,旋转后合成为复数谐波图;In this embodiment, when the system function harmonic diagrams of different orders are rotated, they are decomposed into real part harmonic diagrams and imaginary part harmonic diagrams, and synthesized into complex harmonic diagrams after rotation;

旋转不同阶的系统函数谐波图后保持图像大小不变,无像素点处使用零填充,非网格像素点处使用插值方法取整。Keep the size of the image unchanged after rotating the harmonic diagram of the system function of different orders, use zero padding at the non-grid pixel points, and use the interpolation method to round the non-grid pixel points.

各旋转角度下的系统矩阵表示为{A1,A2, ..., AN}。The system matrix under each rotation angle is expressed as {A 1, A 2 , ..., A N }.

步骤S500,将所述观测向量序列按列进行合并、将各旋转角度下的系统矩阵按列进行合并,合并后,构建线性方程组;对所述线性方程组求解,得到待成像的目标对象对应重建的磁粒子图像。Step S500, combining the observation vector sequence by column, merging the system matrices under each rotation angle by column, and constructing a linear equation system after merging; solving the linear equation system to obtain the corresponding Reconstructed magnetic particle image.

在本实施例中,构建线性方程组,其方法为:In this embodiment, construct linear equation system, its method is:

; ; ;

其中,表示各旋转角度下的系统矩阵{A1,A2, ..., AN}按列进行合并系统矩阵,表示所述观测向量序列{b1, b2, ..., bN}中所有观测向量按列合并后的观测向量,表示待成像的目标物体的离散向量形式。in, Represents the system matrix {A 1, A 2 , ..., A N } at each rotation angle to merge the system matrix by column, Represents the observation vector after all the observation vectors in the observation vector sequence {b 1 , b 2 , ..., b N } are merged by columns, A discrete vector form representing the target object to be imaged.

然后,对所述线性方程组求解,得到待成像的目标对象对应重建的磁粒子图像。Then, the linear equations are solved to obtain a reconstructed magnetic particle image corresponding to the target object to be imaged.

其中,在对线性方程组求解时,优选使用正则化迭代求解算法,具体为:使用L2范数建立目标函数,使用kaczmarz算法迭代求解。论文中的技术方法:使用L1范数和TV范数建立目标函数,使用ADMM算法迭代求解。Among them, when solving the linear equation system, it is preferable to use a regularized iterative solution algorithm, specifically: use the L2 norm to establish an objective function, and use the kaczmarz algorithm to iteratively solve it. The technical method in the paper: use the L1 norm and TV norm to establish the objective function, and use the ADMM algorithm to iteratively solve it.

另外,为了更一步验证本发明方法的有效性,下述进行举例说明。In addition, in order to further verify the effectiveness of the method of the present invention, an example is given below.

本实施例中基于磁场自由线的磁粒子成像装置优选采用开放式磁场自由线磁粒子成像系统,其中,成像视野大小半径设置为20毫米,基于磁场自由线的磁粒子成像方式如图3所示为旋转磁场自由线或旋转被测物体。选择磁场HSF梯度设置为1T/m,驱动磁场使用高频低幅正弦交变磁场HDF, 聚焦磁场HFF使用低频高幅正弦交变磁场,合成磁粒子成像系统磁场H=HSF+HDF+HFFIn this embodiment, the magnetic particle imaging device based on free lines of magnetic field preferably adopts an open free line of magnetic field magnetic particle imaging system, wherein the radius of the imaging field of view is set to 20 mm, and the magnetic particle imaging method based on free lines of magnetic field is shown in Figure 3 Free line of rotating magnetic field or rotating object to be measured. Select the magnetic field H SF gradient to be set to 1T/m, the driving magnetic field uses a high-frequency low-amplitude sinusoidal alternating magnetic field H DF , the focusing magnetic field H FF uses a low-frequency high-amplitude sinusoidal alternating magnetic field, and the synthetic magnetic particle imaging system magnetic field H=H SF +H DF + H FF .

其中,驱动磁场幅值为ADF=8mT、频率为fDF=2500赫兹,即Among them, the amplitude of the driving magnetic field is A DF =8mT, and the frequency is f DF =2500 Hz, namely

                           (1) (1)

聚焦磁场幅值为AFF=14mT、频率为fDF=20赫兹,即The amplitude of the focusing magnetic field is A FF =14mT, and the frequency is f DF =20 Hz, namely

                          (2) (2)

数字采样过程中采样率为1兆赫兹,采样时间为1秒。使用三轴位移台作为测量系统矩阵的测量装置,测试系统矩阵大小设置为20行20列,每个像素大小为2毫米。The sampling rate in the digital sampling process is 1 MHz, and the sampling time is 1 second. A three-axis translation stage is used as the measurement device for the measurement system matrix. The size of the test system matrix is set to 20 rows and 20 columns, and the size of each pixel is 2 mm.

测试使用粒子为超顺磁纳米氧化铁粒子,粒子模型可粗略理解为绝热郎之万模型描述的粒子:,其中为粒子本身性质与测量环境参数。The particles used in the test are superparamagnetic nano-iron oxide particles, and the particle model can be roughly understood as the particles described by the adiabatic Langevin model: ,in For the properties of the particle itself and the measurement of environmental parameters.

然后先固定位移台,将磁粒子成像装置适当远离位移台,以当前位移台探测杆的方向为初始方向,即0°,测量系统矩阵时按照先列后行的轨迹移动测试样本(即待成像的目标物体),单位样本设置为2毫米立方的装有测试粒子原液浓度的载液腔体,开启基于磁场自由线的磁粒子成像装置。Then fix the translation stage first, move the magnetic particle imaging device away from the translation platform appropriately, and take the direction of the detection rod of the current translation platform as the initial direction, that is, 0°. When measuring the system matrix, move the test sample (that is, The target object), the unit sample is set to a 2 mm cubic liquid-carrying cavity filled with the concentration of the test particle stock solution, and the magnetic particle imaging device based on the free line of the magnetic field is turned on.

测量每一个像素处单位样本的信号,使用快速傅里叶变换得到频谱图,根据成像装置信噪比选择2、3、4、5、6、7阶谐波作为粒子信号,基频信号考虑到直接馈通干扰被排除。测试完成像视野内所有像素点的信号后,分别建立2、3、4、5、6、7阶粒子信号的谐波图。Measure the signal of the unit sample at each pixel, use the fast Fourier transform to obtain the spectrogram, select the 2nd, 3rd, 4th, 5th, 6th, and 7th order harmonics as the particle signal according to the signal-to-noise ratio of the imaging device, and take into account the fundamental frequency signal Direct feedthrough interference is excluded. After testing the signals of all pixels in the field of view, the harmonic diagrams of the 2nd, 3rd, 4th, 5th, 6th, and 7th order particle signals are respectively established.

以shepp-logan头模型作为标准测试仿体,如图6中的(a)所示,旋转顺序设置为顺时针方向,3.6°步进角,共旋转50个角度。按照旋转顺序旋转shepp-logan头模型,每个角度下测量粒子响应的信号,使用2、3、4、5、6、7阶谐波建立观测向量{b1, b2, ..., bN}。Taking the shepp-logan head model as the standard test phantom, as shown in (a) in Figure 6, the rotation sequence is set to clockwise, with a step angle of 3.6°, and a total of 50 angles are rotated. Rotate the shepp-logan head model according to the rotation sequence, measure the signal of the particle response at each angle, and use the 2, 3, 4, 5, 6, 7 order harmonics to establish the observation vector {b 1 , b 2 , ..., b N }.

按照相同的旋转角度顺序,将根据初始角度下的系统矩阵建立的各阶系统函数谐波图进行旋转,如图4中(b)所示,得到所有角度下的系统函数谐波图。传统方法构建系统举证,如图4中(a)所示。According to the same order of rotation angles, the system function harmonic diagrams of each order established according to the system matrix at the initial angle are rotated, as shown in (b) in Figure 4, and the system function harmonic diagrams at all angles are obtained. The traditional method of building a system proof, as shown in (a) in Figure 4.

如图5中的(a)、(b)、(c)为初始角度、旋转36°、旋转72°(即旋转角度1、旋转角度2、旋转角度3,图4中的同理)的粒子信号2、3、4阶谐波图。将各阶谐波图建立为对应角度下的系统矩阵{A1,A2, ..., AN}。(a), (b), and (c) in Figure 5 are particles with initial angles, 36° rotation, and 72° rotation (that is, rotation angle 1, rotation angle 2, and rotation angle 3, the same as in Figure 4) Signal 2, 3, 4 order harmonic diagram. The harmonic diagram of each order is established as the system matrix {A 1, A 2 , ..., A N } under the corresponding angle.

将所有系统矩阵按列合并为系统矩阵A,将所有观测向量按列合并为观测向量b,建立待测物体的成像系统线性方程组,并使用正则化kaczmarz方法求解线性方程组,正则化参数设置为0.001,迭代次数设置为1000次,得到x。最后将x重排为待成像的目标物体的图像,如图6中的(b)所示。Merge all system matrices into system matrix A by columns, merge all observation vectors into observation vector b by columns, establish the linear equations of the imaging system of the object to be measured, and use the regularized kaczmarz method to solve the linear equations, and set the regularization parameters is 0.001, the number of iterations is set to 1000, and x is obtained. Finally, x is rearranged into the image of the target object to be imaged, as shown in (b) in Fig. 6 .

本发明第二实施例的一种基于旋转谐波图的磁场自由线磁粒子成像系统,如图2所示,该系统包括:初始化设置模块100、谐波图构建模块200、观测向量构建模块300、系统矩阵构建模块400、图像重建模块500;A magnetic field free-line magnetic particle imaging system based on a rotating harmonic diagram according to the second embodiment of the present invention, as shown in FIG. 2 , the system includes: an initialization setting module 100, a harmonic diagram construction module 200, and an observation vector construction module 300 , system matrix construction module 400, image reconstruction module 500;

所述初始化设置模块100,配置为设置所述磁粒子成像装置的相关参数,开启并运行所述基于磁场自由线的磁粒子成像装置;所述相关参数包括成像视野半径大小、选择磁场梯度、激励磁场幅值与频率、数字采样频率与时间、单位样本大小;The initialization setting module 100 is configured to set the relevant parameters of the magnetic particle imaging device, start and run the magnetic particle imaging device based on free lines of magnetic field; the relevant parameters include imaging field of view radius, selection of magnetic field gradient, excitation Magnetic field amplitude and frequency, digital sampling frequency and time, unit sample size;

所述谐波图构建模块200,配置为设置所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置的位置与方向,并结合所述成像视野半径,设置单位样本的移动路径;按照设定的移动路径移动单位样本,测量所述基于磁场自由线的磁粒子成像装置成像视野范围内每一个像素处单位样本的信号,进而构建不同阶的系统函数谐波图;所述系统矩阵测量装置为根据设定移动路径将单位样本移动至指定位置的装置;The harmonic diagram construction module 200 is configured to set the position and direction of the system matrix measurement device in the magnetic particle imaging device based on free lines of magnetic field, and combine the imaging field of view radius to set the movement path of the unit sample; according to the design Move the unit sample with a predetermined moving path, measure the signal of the unit sample at each pixel within the imaging field of view of the magnetic particle imaging device based on the free line of magnetic field, and then construct the harmonic diagram of the system function of different orders; the system matrix measurement device It is a device that moves the unit sample to a designated position according to a set movement path;

所述观测向量构建模块300,配置为以所述系统矩阵测量装置的方向为初始方向,设置旋转角度以及旋转顺序;按照所述旋转角度及所述旋转顺序旋转所述基于磁场自由线的磁粒子成像装置的磁场自由线或者待成像的目标对象,测量各旋转角度下待成像的目标对象的响应信号并构建观测向量序列;The observation vector construction module 300 is configured to take the direction of the system matrix measuring device as the initial direction, set the rotation angle and the rotation sequence; rotate the magnetic particles based on the free lines of the magnetic field according to the rotation angle and the rotation sequence The magnetic field free line of the imaging device or the target object to be imaged, measuring the response signal of the target object to be imaged at each rotation angle and constructing an observation vector sequence;

所述系统矩阵构建模块400,配置为按照所述旋转角度,旋转不同阶的系统函数谐波图,并基于旋转后的不同阶的系统函数谐波图构建各旋转角度下的系统矩阵;The system matrix construction module 400 is configured to rotate the system function harmonic diagrams of different orders according to the rotation angle, and construct the system matrix at each rotation angle based on the rotated system function harmonic diagrams of different orders;

所述图像重建模块500,配置为将所述观测向量序列按列进行合并、将各旋转角度下的系统矩阵按列进行合并,合并后,构建线性方程组;对所述线性方程组求解,得到待成像的目标对象对应重建的磁粒子图像。The image reconstruction module 500 is configured to combine the observation vector sequence by column, combine the system matrices under each rotation angle by column, and construct a linear equation system after the combination; solve the linear equation system to obtain The target object to be imaged corresponds to the reconstructed magnetic particle image.

所述技术领域的技术人员可以清楚的了解到,为描述的方便和简洁,上述描述的系统的具体的工作过程及有关说明,可以参考前述方法实施例中的对应过程,在此不再赘述。Those skilled in the technical field can clearly understand that for the convenience and brevity of the description, the specific working process and relevant descriptions of the above-described system can refer to the corresponding process in the foregoing method embodiments, and will not be repeated here.

需要说明的是,上述实施例提供的基于旋转谐波图的磁场自由线磁粒子成像系统,仅以上述各功能模块的划分进行举例说明,在实际应用中,可以根据需要而将上述功能分配由不同的功能模块来完成,即将本发明实施例中的模块或者步骤再分解或者组合,例如,上述实施例的模块可以合并为一个模块,也可以进一步拆分成多个子模块,以完成以上描述的全部或者部分功能。对于本发明实施例中涉及的模块、步骤的名称,仅仅是为了区分各个模块或者步骤,不视为对本发明的不当限定。It should be noted that the magnetic field free line magnetic particle imaging system based on the rotating harmonic diagram provided in the above embodiment is only illustrated by the division of the above functional modules. In practical applications, the above functions can be allocated by different functional modules, that is, to decompose or combine the modules or steps in the embodiments of the present invention. For example, the modules in the above embodiments can be combined into one module, or can be further split into multiple sub-modules to complete the above-described full or partial functionality. The names of the modules and steps involved in the embodiments of the present invention are only used to distinguish each module or step, and are not regarded as improperly limiting the present invention.

本发明第三实施例的一种电子设备,至少一个处理器;以及与至少一个所述处理器通信连接的存储器;其中,所述存储器存储有可被所述处理器执行的指令,所述指令用于被所述处理器执行以实现权利要求上述的基于旋转谐波图的磁场自由线磁粒子成像方法。An electronic device according to the third embodiment of the present invention includes at least one processor; and a memory communicatively connected to at least one of the processors; wherein, the memory stores instructions executable by the processor, and the instructions It is used to be executed by the processor to realize the magnetic particle imaging method based on the rotational harmonic diagram of the above-mentioned claims.

本发明第四实施例的一种计算机可读存储介质,所述计算机可读存储介质存储有计算机指令,所述计算机指令用于被所述计算机执行以实现上述的基于旋转谐波图的磁场自由线磁粒子成像方法。A computer-readable storage medium according to the fourth embodiment of the present invention, the computer-readable storage medium stores computer instructions, and the computer instructions are used to be executed by the computer to realize the above-mentioned magnetic field freedom based on the rotation harmonic diagram Line Magnetic Particle Imaging Methods.

所述技术领域的技术人员可以清楚的了解到,为描述的方便和简洁,上述描述的电子设备、计算机可读存储介质的具体工作过程及有关说明,可以参考前述方法实例中的对应过程,在此不再赘述。Those skilled in the technical field can clearly understand that for the convenience and brevity of the description, the specific working process and related instructions of the electronic device and the computer-readable storage medium described above can refer to the corresponding process in the aforementioned method example. This will not be repeated here.

下面参考图7,其示出了适于用来实现本申请方法、系统、装置实施例的服务器的计算机系统的结构示意图。图7示出的服务器仅仅是一个示例,不应对本申请实施例的功能和使用范围带来任何限制。Referring now to FIG. 7 , it shows a schematic structural diagram of a server computer system suitable for implementing the method, system, and device embodiments of the present application. The server shown in FIG. 7 is only an example, and should not limit the functions and scope of use of this embodiment of the present application.

如图7所示,计算机系统包括中央处理单元(CPU,Central Processing Unit)701,其可以根据存储在只读存储器(ROM,Read Only Memory)702中的程序或者从存储部分708加载到随机访问存储器(RAM,Random Access Memory)703中的程序而执行各种适当的动作和处理。在RAM 703中,还存储有系统操作所需的各种程序和数据。CPU701、ROM702以及RAM703通过总线704彼此相连。输入/输出(I/O,Input/Output)接口705也连接至总线704。As shown in Figure 7, the computer system includes a central processing unit (CPU, Central Processing Unit) 701, which can be stored in a program in a read-only memory (ROM, Read Only Memory) 702 or loaded into a random access memory from a storage section 708 (RAM, Random Access Memory) 703 to execute various appropriate actions and processing. In RAM 703, various programs and data necessary for system operation are also stored. The CPU 701 , ROM 702 , and RAM 703 are connected to each other via a bus 704 . An input/output (I/O, Input/Output) interface 705 is also connected to the bus 704 .

以下部件连接至I/O接口705:包括键盘、鼠标等的输入部分706;包括诸如阴极射线管(CRT,Cathode Ray Tube)、液晶显示器(LCD,Liquid Crystal Display)等以及扬声器等的输出部分707;包括硬盘等的存储部分708;以及包括诸如LAN(局域网,Local AreaNetwork)卡、调制解调器等的网络接口卡的通讯部分709。通讯部分709经由诸如因特网的网络执行通信处理。驱动器710也根据需要连接至I/O接口705。可拆卸介质711,诸如磁盘、光盘、磁光盘、半导体存储器等等,根据需要安装在驱动器710上,以便于从其上读出的计算机程序根据需要被安装入存储部分708。The following components are connected to the I/O interface 705: an input section 706 including a keyboard, a mouse, etc.; an output section 707 including a cathode ray tube (CRT, Cathode Ray Tube), a liquid crystal display (LCD, Liquid Crystal Display) etc., and a speaker ; a storage section 708 comprising a hard disk, etc.; and a communication section 709 comprising network interface cards such as LAN (Local Area Network, Local Area Network) cards, modems, etc. The communication section 709 performs communication processing via a network such as the Internet. A drive 710 is also connected to the I/O interface 705 as needed. A removable medium 711 such as a magnetic disk, optical disk, magneto-optical disk, semiconductor memory, etc. is mounted on the drive 710 as necessary so that a computer program read therefrom is installed into the storage section 708 as necessary.

特别地,根据本公开的实施例,上文参考流程图描述的过程可以被实现为计算机软件程序。例如,本公开的实施例包括一种计算机程序产品,其包括承载在计算机可读介质上的计算机程序,该计算机程序包含用于执行流程图所示的方法的程序代码。在这样的实施例中,该计算机程序可以通过通讯部分709从网络上被下载和安装,和/或从可拆卸介质711被安装。在该计算机程序被中央处理单元(CPU701执行时,执行本申请的方法中限定的上述功能。需要说明的是,本申请上述的计算机可读介质可以是计算机可读信号介质或者计算机可读存储介质或者是上述两者的任意组合。计算机可读存储介质例如可以是——但不限于——电、磁、光、电磁、红外线、或半导体的系统、装置或器件,或者任意以上的组合。计算机可读存储介质的更具体的例子可以包括但不限于:具有一个或多个导线的电连接、便携式计算机磁盘、硬盘、随机访问存储器(RAM)、只读存储器(ROM)、可擦式可编程只读存储器(EPROM或闪存)、光纤、便携式紧凑磁盘只读存储器(CD-ROM)、光存储器件、磁存储器件、或者上述的任意合适的组合。在本申请中,计算机可读存储介质可以是任何包含或存储程序的有形介质,该程序可以被指令执行系统、装置或者器件使用或者与其结合使用。而在本申请中,计算机可读的信号介质可以包括在基带中或者作为载波一部分传播的数据信号,其中承载了计算机可读的程序代码。这种传播的数据信号可以采用多种形式,包括但不限于电磁信号、光信号或上述的任意合适的组合。计算机可读的信号介质还可以是计算机可读存储介质以外的任何计算机可读介质,该计算机可读介质可以发送、传播或者传输用于由指令执行系统、装置或者器件使用或者与其结合使用的程序。计算机可读介质上包含的程序代码可以用任何适当的介质传输,包括但不限于:无线、电线、光缆、RF等等,或者上述的任意合适的组合。In particular, according to an embodiment of the present disclosure, the processes described above with reference to the flowcharts can be implemented as computer software programs. For example, embodiments of the present disclosure include a computer program product, which includes a computer program carried on a computer-readable medium, where the computer program includes program codes for executing the methods shown in the flowcharts. In such an embodiment, the computer program may be downloaded and installed from a network via communication portion 709 and/or installed from removable media 711 . When the computer program is executed by the central processing unit (CPU701), the above-mentioned functions defined in the method of the present application are executed. It should be noted that the computer-readable medium mentioned above in the present application can be a computer-readable signal medium or a computer-readable storage medium Or any combination of the above two. Computer-readable storage media can be, for example—but not limited to—electric, magnetic, optical, electromagnetic, infrared, or semiconductor systems, devices, or devices, or any combination of the above. Computer More specific examples of readable storage media may include, but are not limited to, electrical connections with one or more wires, portable computer diskettes, hard disks, random access memory (RAM), read only memory (ROM), erasable programmable Read-only memory (EPROM or flash memory), optical fiber, portable compact disk read-only memory (CD-ROM), optical storage device, magnetic storage device, or any suitable combination of the above. In this application, the computer-readable storage medium can be Is any tangible medium that contains or stores a program that can be used by or in conjunction with an instruction execution system, device, or device. In this application, a computer-readable signal medium can be included in the baseband or propagated as part of a carrier wave A data signal, which carries computer-readable program code. This propagated data signal can take a variety of forms, including but not limited to electromagnetic signals, optical signals, or any suitable combination of the above. Computer-readable signal media can also Any computer-readable medium, other than a computer-readable storage medium, that can send, propagate, or transmit a program for use by or in conjunction with an instruction execution system, apparatus, or device. Contained on a computer-readable medium Program code may be transmitted using any suitable medium, including but not limited to: wireless, wire, optical fiber cable, RF, etc., or any suitable combination of the above.

可以以一种或多种程序设计语言或其组合来编写用于执行本申请的操作的计算机程序代码,上述程序设计语言包括面向对象的程序设计语言—诸如Java、Smalltalk、C++,还包括常规的过程式程序设计语言—诸如“C”语言或类似的程序设计语言。程序代码可以完全地在用户计算机上执行、部分地在用户计算机上执行、作为一个独立的软件包执行、部分在用户计算机上部分在远程计算机上执行、或者完全在远程计算机或服务器上执行。在涉及远程计算机的情形中,远程计算机可以通过任意种类的网络——包括局域网(LAN)或广域网(WAN)—连接到用户计算机,或者,可以连接到外部计算机(例如利用因特网服务提供商来通过因特网连接)。Computer program code for performing the operations of the present application may be written in one or more programming languages or combinations thereof, including object-oriented programming languages—such as Java, Smalltalk, C++, and conventional Procedural Programming Language - such as "C" or a similar programming language. The program code may execute entirely on the user's computer, partly on the user's computer, as a stand-alone software package, partly on the user's computer and partly on a remote computer or entirely on the remote computer or server. In cases involving a remote computer, the remote computer can be connected to the user computer through any kind of network, including a local area network (LAN) or a wide area network (WAN), or it can be connected to an external computer (such as through an Internet service provider). Internet connection).

附图中的流程图和框图,图示了按照本申请各种实施例的系统、方法和计算机程序产品的可能实现的体系架构、功能和操作。在这点上,流程图或框图中的每个方框可以代表一个模块、程序段、或代码的一部分,该模块、程序段、或代码的一部分包含一个或多个用于实现规定的逻辑功能的可执行指令。也应当注意,在有些作为替换的实现中,方框中所标注的功能也可以以不同于附图中所标注的顺序发生。例如,两个接连地表示的方框实际上可以基本并行地执行,它们有时也可以按相反的顺序执行,这依所涉及的功能而定。也要注意的是,框图和/或流程图中的每个方框、以及框图和/或流程图中的方框的组合,可以用执行规定的功能或操作的专用的基于硬件的系统来实现,或者可以用专用硬件与计算机指令的组合来实现。The flowchart and block diagrams in the Figures illustrate the architecture, functionality, and operation of possible implementations of systems, methods and computer program products according to various embodiments of the present application. In this regard, each block in a flowchart or block diagram may represent a module, program segment, or portion of code that contains one or more logical functions for implementing specified executable instructions. It should also be noted that, in some alternative implementations, the functions noted in the block may occur out of the order noted in the figures. For example, two blocks shown in succession may, in fact, be executed substantially concurrently, or they may sometimes be executed in the reverse order, depending upon the functionality involved. It should also be noted that each block of the block diagrams and/or flowchart illustrations, and combinations of blocks in the block diagrams and/or flowchart illustrations, can be implemented by a dedicated hardware-based system that performs the specified functions or operations , or may be implemented by a combination of dedicated hardware and computer instructions.

术语“第一”、 “第二”等是用于区别类似的对象,而不是用于描述或表示特定的顺序或先后次序。The terms "first", "second", etc. are used to distinguish similar items, and are not used to describe or represent a specific order or sequence.

术语“包括”或者任何其它类似用语旨在涵盖非排他性的包含,从而使得包括一系列要素的过程、方法、物品或者设备/装置不仅包括那些要素,而且还包括没有明确列出的其它要素,或者还包括这些过程、方法、物品或者设备/装置所固有的要素。The term "comprising" or any other similar term is intended to cover a non-exclusive inclusion such that a process, method, article, or apparatus/apparatus comprising a set of elements includes not only those elements but also other elements not expressly listed, or Also included are elements inherent in these processes, methods, articles, or devices/devices.

至此,已经结合附图所示的优选实施方式描述了本发明的技术方案,但是,本领域技术人员容易理解的是,本发明的保护范围显然不局限于这些具体实施方式。在不偏离本发明的原理的前提下,本领域技术人员可以对相关技术特征作出等同的更改或替换,这些更改或替换之后的技术方案都将落入本发明的保护范围之内。So far, the technical solutions of the present invention have been described in conjunction with the preferred embodiments shown in the accompanying drawings, but those skilled in the art will easily understand that the protection scope of the present invention is obviously not limited to these specific embodiments. Without departing from the principles of the present invention, those skilled in the art can make equivalent changes or substitutions to relevant technical features, and the technical solutions after these changes or substitutions will all fall within the protection scope of the present invention.

Claims (9)

1.一种基于旋转谐波图的磁场自由线磁粒子成像方法,应用于基于磁场自由线的磁粒子成像装置,其特征在于,该方法包括:1. A method for magnetic particle imaging based on free lines of magnetic field based on rotational harmonic diagrams, applied to a magnetic particle imaging device based on free lines of magnetic field, characterized in that the method comprises: 步骤S100,设置所述基于磁场自由线的磁粒子成像装置的相关参数,开启并运行所述基于磁场自由线的磁粒子成像装置;所述相关参数包括成像视野半径大小、选择磁场梯度、激励磁场幅值与频率、数字采样频率与时间、单位样本大小;Step S100, setting the relevant parameters of the magnetic particle imaging device based on free lines of magnetic field, starting and running the magnetic particle imaging device based on free lines of magnetic field; the relevant parameters include imaging field of view radius, selected magnetic field gradient, excitation magnetic field Amplitude and frequency, digital sampling frequency and time, unit sample size; 步骤S200,设置所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置的位置与方向,并结合所述成像视野半径,设置单位样本的移动路径;按照设定的移动路径移动单位样本,测量所述基于磁场自由线的磁粒子成像装置成像视野范围内每一个像素处单位样本的信号,进而构建不同阶的系统函数谐波图;所述系统矩阵测量装置为根据设定移动路径将单位样本移动至指定位置的装置;Step S200, setting the position and direction of the system matrix measuring device in the magnetic particle imaging device based on free lines of magnetic field, and combining the imaging field of view radius, setting the moving path of the unit sample; moving the unit sample according to the set moving path, Measure the signal of the unit sample at each pixel within the imaging field of view of the magnetic particle imaging device based on the free lines of the magnetic field, and then construct system function harmonic diagrams of different orders; A device for moving samples to designated locations; 步骤S300,以所述系统矩阵测量装置的方向为初始方向,设置旋转角度以及旋转顺序;按照所述旋转角度及所述旋转顺序旋转所述基于磁场自由线的磁粒子成像装置的磁场自由线或者待成像的目标对象,测量各旋转角度下待成像的目标对象的响应信号并构建观测向量序列;Step S300, taking the direction of the system matrix measuring device as the initial direction, setting the rotation angle and the rotation sequence; rotating the magnetic field free lines of the magnetic particle imaging device based on the magnetic field free lines or The target object to be imaged, measuring the response signal of the target object to be imaged at each rotation angle and constructing an observation vector sequence; 步骤S400,按照所述旋转角度,旋转不同阶的系统函数谐波图,并基于旋转后的不同阶的系统函数谐波图构建各旋转角度下的系统矩阵;Step S400, according to the rotation angle, rotate the harmonic diagram of the system function of different orders, and construct the system matrix under each rotation angle based on the rotated harmonic diagram of the system function of different orders; 步骤S500,将所述观测向量序列按列进行合并、将各旋转角度下的系统矩阵按列进行合并,合并后,构建线性方程组;对所述线性方程组求解,得到待成像的目标对象对应重建的磁粒子图像。Step S500, combining the observation vector sequence by column, merging the system matrices under each rotation angle by column, and constructing a linear equation system after merging; solving the linear equation system to obtain the corresponding Reconstructed magnetic particle image. 2.根据权利要求1所述的基于旋转谐波图的磁场自由线磁粒子成像方法,其特征在于,测量所述基于磁场自由线的磁粒子成像装置成像视野范围内每一个像素处单位样本的信号,进而构建不同阶的系统函数谐波图,其方法为:2. the magnetic particle imaging method based on the free line of magnetic field free line according to claim 1, is characterized in that, measure the unit sample at each pixel place in the magnetic particle imaging device imaging field of view based on the free line of magnetic field Signal, and then construct the harmonic diagram of the system function of different order, the method is as follows: 测量每一个像素处单位样本的时域信号,并通过快速傅里叶变换得到频谱;Measure the time-domain signal of the unit sample at each pixel, and obtain the frequency spectrum through fast Fourier transform; 根据所述基于磁场自由线的磁粒子成像装置的信噪比,筛选信噪比大于设定信噪比阈值的谐波信号,将筛选后的谐波信号作为第一谐波信号;基于所述频谱,将各像素处相同阶的第一谐波信号进行合成,得到不同阶的系统函数谐波图。According to the signal-to-noise ratio of the magnetic particle imaging device based on the free line of magnetic field, filter the harmonic signal whose signal-to-noise ratio is greater than the set signal-to-noise ratio threshold, and use the filtered harmonic signal as the first harmonic signal; based on the said Spectrum, the first harmonic signals of the same order at each pixel are synthesized to obtain system function harmonic diagrams of different orders. 3.根据权利要求2所述的基于旋转谐波图的磁场自由线磁粒子成像方法,其特征在于,设置旋转角度以及旋转顺序,其方法为:3. the magnetic field free line magnetic particle imaging method based on rotating harmonic diagram according to claim 2, is characterized in that, setting rotation angle and rotation order, its method is: 以所述初始方向为0°,按照等间距或不等间距方式步进旋转至180°,保证磁场自由线的运动范围能够覆盖全部成像视野,共旋转N个角度;其中,N表示设定数量。Taking the initial direction as 0°, stepping and rotating to 180° according to equal intervals or unequal intervals, ensuring that the range of motion of the free line of the magnetic field can cover the entire imaging field of view, and rotate N angles in total; where N represents the set number . 4.根据权利要求3所述的基于旋转谐波图的磁场自由线磁粒子成像方法,其特征在于,测量各旋转角度下待成像的目标对象的响应信号并构建观测向量序列,其方法为:4. the magnetic field free line magnetic particle imaging method based on rotating harmonic diagram according to claim 3, it is characterized in that, measure the response signal of the target object to be imaged under each rotation angle and construct observation vector sequence, its method is: 测量各旋转角度下待成像的目标对象的响应信号并构建当前旋转角度下的观测列向量,进而构建所有旋转角度下的观测向量序列;Measure the response signal of the target object to be imaged at each rotation angle and construct the observation column vector at the current rotation angle, and then construct the observation vector sequence at all rotation angles; 所述观测列向量为根据所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置初始方向下的系统矩阵使用的特征谐波提取对应旋转角度下待成像的目标物体的响应信号的特征谐波构建的列向量。The observation column vector is the characteristic harmonic used to extract the response signal of the target object to be imaged at the corresponding rotation angle according to the characteristic harmonic used by the system matrix in the initial direction of the system matrix measuring device in the magnetic particle imaging device based on free lines of magnetic field Column vector of wave builds. 5.根据权利要求1所述的基于旋转谐波图的磁场自由线磁粒子成像方法,其特征在于,在旋转不同阶的系统函数谐波图时分解为实部谐波图、虚部谐波图,旋转后合成为复数谐波图;5. the magnetic field free line magnetic particle imaging method based on rotating harmonic diagram according to claim 1, is characterized in that, when rotating the system function harmonic diagram of different orders, it is decomposed into real part harmonic diagram, imaginary part harmonic graph, synthesized into a complex harmonic graph after rotation; 旋转不同阶的系统函数谐波图后保持图像大小不变,无像素点处使用零填充,非网格像素点处使用插值方法取整。Keep the size of the image unchanged after rotating the harmonic diagram of the system function of different orders, use zero padding at the non-grid pixel points, and use the interpolation method to round the non-grid pixel points. 6.根据权利要求1所述的基于旋转谐波图的磁场自由线磁粒子成像方法,其特征在于,构建线性方程组,其方法为:;其中,表示各旋转角度下的系统矩阵{A1, A2, ..., AN}按列进行合并系统矩阵,表示所述观测向量序列{b1, b2,..., bN}中所有观测向量按列合并后的观测向量,表示待成像的目标物体的离散向量形式。6. the magnetic field free line magnetic particle imaging method based on rotating harmonic diagram according to claim 1, is characterized in that, constructs linear equations, its method is: ; ; ;in, Represents the system matrix {A 1, A 2 , ..., A N } at each rotation angle to merge the system matrix by column, Represents the observation vector after all the observation vectors in the observation vector sequence {b 1 , b 2 ,..., b N } are merged by columns, A discrete vector form representing the target object to be imaged. 7.一种基于旋转谐波图的磁场自由线磁粒子成像系统,基于权利要求1-6任一项所述的基于旋转谐波图的磁场自由线磁粒子成像方法,其特征在于,该系统包括:初始化设置模块、谐波图构建模块、观测向量构建模块、系统矩阵构建模块、图像重建模块;7. A magnetic field free-line magnetic particle imaging system based on a rotational harmonic diagram, based on the magnetic field free-line magnetic particle imaging method based on a rotational harmonic diagram according to any one of claims 1-6, characterized in that the system Including: initialization setting module, harmonic diagram building module, observation vector building module, system matrix building module, image reconstruction module; 所述初始化设置模块,配置为设置所述基于磁场自由线的磁粒子成像装置的相关参数,开启并运行所述基于磁场自由线的磁粒子成像装置;所述相关参数包括成像视野半径大小、选择磁场梯度、激励磁场幅值与频率、数字采样频率与时间、单位样本大小;The initialization setting module is configured to set the relevant parameters of the magnetic particle imaging device based on free lines of magnetic field, start and run the magnetic particle imaging device based on free lines of magnetic field; the relevant parameters include imaging field of view radius, selection Magnetic field gradient, excitation magnetic field amplitude and frequency, digital sampling frequency and time, unit sample size; 所述谐波图构建模块,配置为设置所述基于磁场自由线的磁粒子成像装置中系统矩阵测量装置的位置与方向,并结合所述成像视野半径,设置单位样本的移动路径;按照设定的移动路径移动单位样本,测量所述基于磁场自由线的磁粒子成像装置成像视野范围内每一个像素处单位样本的信号,进而构建不同阶的系统函数谐波图;所述系统矩阵测量装置为根据设定移动路径将单位样本移动至指定位置的装置;The harmonic diagram construction module is configured to set the position and direction of the system matrix measurement device in the magnetic particle imaging device based on free lines of magnetic field, and combine the imaging field of view radius to set the moving path of the unit sample; according to the setting Move the unit sample according to the moving path, measure the signal of the unit sample at each pixel within the imaging field of view of the magnetic particle imaging device based on the free line of magnetic field, and then construct the harmonic diagram of the system function of different orders; the system matrix measurement device is A device that moves a unit sample to a designated location according to a set movement path; 所述观测向量构建模块,配置为以所述系统矩阵测量装置的方向为初始方向,设置旋转角度以及旋转顺序;按照所述旋转角度及所述旋转顺序旋转所述基于磁场自由线的磁粒子成像装置的磁场自由线或者待成像的目标对象,测量各旋转角度下待成像的目标对象的响应信号并构建观测向量序列;The observation vector construction module is configured to take the direction of the system matrix measurement device as the initial direction, set the rotation angle and the rotation sequence; rotate the magnetic particle imaging based on the free line of the magnetic field according to the rotation angle and the rotation sequence The free line of the magnetic field of the device or the target object to be imaged, measuring the response signal of the target object to be imaged at each rotation angle and constructing an observation vector sequence; 所述系统矩阵构建模块,配置为按照所述旋转角度,旋转不同阶的系统函数谐波图,并基于旋转后的不同阶的系统函数谐波图构建各旋转角度下的系统矩阵;The system matrix construction module is configured to rotate the system function harmonic diagrams of different orders according to the rotation angle, and construct the system matrix at each rotation angle based on the rotated system function harmonic diagrams of different orders; 所述图像重建模块,配置为将所述观测向量序列按列进行合并、将各旋转角度下的系统矩阵按列进行合并,合并后,构建线性方程组;对所述线性方程组求解,得到待成像的目标对象对应重建的磁粒子图像。The image reconstruction module is configured to combine the observation vector sequence by column, and combine the system matrices under each rotation angle by column. After the combination, construct a linear equation system; solve the linear equation system to obtain The imaged target object corresponds to the reconstructed magnetic particle image. 8.一种电子设备,其特征在于,包括:8. An electronic device, characterized in that it comprises: 至少一个处理器;以及与至少一个所述处理器通信连接的存储器;at least one processor; and memory communicatively coupled to at least one of said processors; 其中,所述存储器存储有可被所述处理器执行的指令,所述指令用于被所述处理器执行以实现权利要求1-6任一项所述的基于旋转谐波图的磁场自由线磁粒子成像方法。Wherein, the memory stores instructions that can be executed by the processor, and the instructions are used to be executed by the processor to realize the free line of magnetic field based on the rotating harmonic diagram according to any one of claims 1-6. Magnetic Particle Imaging Methods. 9.一种计算机可读存储介质,其特征在于,所述计算机可读存储介质存储有计算机指令,所述计算机指令用于被所述计算机执行以实现权利要求1-6任一项所述的基于旋转谐波图的磁场自由线磁粒子成像方法。9. A computer-readable storage medium, characterized in that the computer-readable storage medium stores computer instructions, and the computer instructions are used to be executed by the computer to implement the method described in any one of claims 1-6. Free-line magnetic particle imaging method for magnetic field based on rotational harmonic map.
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