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CN108346150A - A kind of cortex thickness method of estimation based on atlas analysis - Google Patents

A kind of cortex thickness method of estimation based on atlas analysis Download PDF

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CN108346150A
CN108346150A CN201810180863.XA CN201810180863A CN108346150A CN 108346150 A CN108346150 A CN 108346150A CN 201810180863 A CN201810180863 A CN 201810180863A CN 108346150 A CN108346150 A CN 108346150A
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cerebral cortex
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王刚
苏庆堂
张小峰
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Abstract

磁共振成像(MRI)的脑皮层厚度估计是研究大脑神经退行性疾病的一项重要技术。本发明提出一种基于图谱分析的脑皮层厚度估计方法,可以有效地捕捉脑皮层的几何形态变化。首先,该方法通过构建四面体网格模型来逼近MRI中的脑皮层形态并反映其内在的几何特性;其次,该方法利用四面体网格中几何约束关系构建Laplace‑Beltramin算子来计算脑皮层内部温度场的分布;最后,通过图谱分析的机理构建由Laplace‑Beltramin算子的特征值和特征向量所表征的热量转移概率表征体系,并追踪最大热量传播概率确定脑皮层温度场内梯度场线的方向与长度,最终获得脑皮层的厚度信息。

Cortical thickness estimation from magnetic resonance imaging (MRI) is an important technique for studying neurodegenerative diseases of the brain. The present invention proposes a method for estimating the thickness of the cerebral cortex based on atlas analysis, which can effectively capture the geometric changes of the cerebral cortex. First, the method approximates the shape of the cerebral cortex in MRI by constructing a tetrahedral mesh model and reflects its intrinsic geometric properties; The distribution of the internal temperature field; finally, construct the heat transfer probability representation system represented by the eigenvalue and eigenvector of the Laplace-Beltramin operator through the mechanism of map analysis, and track the maximum heat transfer probability to determine the gradient field line in the cerebral cortex temperature field The direction and length of the cortex are finally obtained to obtain the thickness information of the cerebral cortex.

Description

一种基于图谱分析的脑皮层厚度估计方法A method for estimating cerebral cortex thickness based on atlas analysis

技术领域technical field

本发明属于计算机应用技术领域,涉及MRI脑皮层形态变化检测技术,用于AD等神经退行性疾病的早期诊断。The invention belongs to the field of computer application technology, relates to MRI cerebral cortex morphology change detection technology, and is used for early diagnosis of neurodegenerative diseases such as AD.

背景技术Background technique

阿尔茨海默病(AD)已成为一种严重危害老年人健康的神经退行性疾病,严重威胁人类健康。为了研发有效的治疗手段阻碍疾病的恶化进程,需要早期对极易转化成AD病症的轻度认知障碍人群(MCI)进行准确诊断,并根据其演化轨迹揭示其病情发展趋势。由于AD病症的出现起始于局部区域,表现为局部区域脑皮层厚度变薄,然后这种现象向大脑其他部分扩散。因此诸多研究人员将脑皮层的厚度变化作为AD病症的辅助诊断依据。为此,采用合适的检测手段提取在局部区域的脑皮层厚度信息一直是本领域内的重要研究课题。Alzheimer's disease (AD) has become a neurodegenerative disease that seriously endangers the health of the elderly and seriously threatens human health. In order to develop effective treatments to hinder the progression of the disease, it is necessary to accurately diagnose the mild cognitive impairment (MCI) population that is easily transformed into AD at an early stage, and reveal the development trend of the disease according to its evolutionary trajectory. Since the appearance of AD symptoms starts in a local area, it is manifested as a thinning of the thickness of the cerebral cortex in the local area, and then this phenomenon spreads to other parts of the brain. Therefore, many researchers regard the thickness change of cerebral cortex as the auxiliary diagnosis basis of AD disease. For this reason, it has been an important research topic in this field to extract the thickness information of the cerebral cortex in a local area by using a suitable detection method.

磁共振成像(MRI)技术可以显示人脑物理参数(如密度)在空间中的分布,并且得到任何方向的断层图像、三维体图像,因此目前已广泛用于AD等神经退行性疾病的早期诊断和揭示其演化过程。该技术结合计算机图形学技术可以量化和评估大脑皮层的微小形态变化,是面向临床无损伤揭示脑皮层几何结构变化的分析方法。但对MRI脑皮层形态变化的量化分析中仍然面临如下核心问题:Magnetic resonance imaging (MRI) technology can display the distribution of physical parameters (such as density) of the human brain in space, and obtain tomographic images and three-dimensional volume images in any direction, so it has been widely used in the early diagnosis of neurodegenerative diseases such as AD and reveal its evolution. This technology combined with computer graphics technology can quantify and evaluate the small morphological changes of the cerebral cortex, and is an analytical method for clinically revealing the geometric structure changes of the cerebral cortex without damage. However, the quantitative analysis of MRI cortical morphological changes still faces the following core problems:

1) 如何利用几何形态度量属性生成保持原有MRI影像数据的脑皮层四面体网格模型。降低以往借助立方体网格近似MRI影像数据所带来的拟合误差;1) How to use geometric morphometric properties to generate a tetrahedral mesh model of the cerebral cortex that maintains the original MRI image data. Reduce the fitting error caused by approximating MRI image data with cube grids in the past;

2) 如何借助图谱理论所体现的脑皮层本质几何特征,在原有拉格朗日方法的基础上,提高脑皮层厚度计算的准确度和鲁棒性。降低单纯依靠拉格朗日方法求解厚度信息所带来的计算误差。2) How to improve the accuracy and robustness of cortical thickness calculation on the basis of the original Lagrangian method with the help of the essential geometric characteristics of the cerebral cortex embodied in the map theory. Reduce the calculation error caused by relying solely on the Lagrangian method to solve the thickness information.

发明内容Contents of the invention

本发明的目的是提供一种基于图谱分析理论的脑皮层厚度估计方法,其特征是通过构建脑皮层核磁共振(MRI)图像的四面体网格表征形式和计算调和能量场中的热量传导规律来捕捉MRI脑皮层中的几何信息,具体步骤描述如下:The purpose of the present invention is to provide a method for estimating the thickness of cerebral cortex based on the atlas analysis theory, which is characterized by constructing the tetrahedral grid representation form of the cerebral cortex nuclear magnetic resonance (MRI) image and calculating the heat conduction law in the harmonic energy field. To capture geometric information in the MRI cerebral cortex, the specific steps are described as follows:

第一步:立方体网格生成:在保持边界形状基础上,生成由立方体单元所组成的背景网格;采用基于顶点连接关系的快速行进法计算具有符号特征的背景立方体网格点的空间位置属性,通过边缘面附近网格点的空间位置的概率分布设计自适应调整网格边长的运算规则,以达到拟合大脑皮层的最佳程度;The first step: Cube grid generation: On the basis of maintaining the boundary shape, generate a background grid composed of cube units; use the fast marching method based on the vertex connection relationship to calculate the spatial position attributes of the background cube grid points with symbolic features , through the probability distribution of the spatial position of the grid points near the edge surface, the algorithm for adaptively adjusting the grid side length is designed to achieve the best degree of fitting to the cerebral cortex;

第二步: 四面体网格剖分:分别对处于边缘面和内部顶点背景网格采用金字塔剖分形式和体心立方点阵的剖分形式进行四面体剖分,然后对剖分后的四面体网格进行零值面的切割、整理;Step 2: Tetrahedral meshing: Tetrahedral meshing is carried out on the edge face and internal vertex background mesh respectively in the form of pyramid splitting and body-centered cubic lattice, and then the four faces after splitting The volume grid is used to cut and organize the zero value surface;

第三步:四面体网格优化:利用基于空间位移梯度张量的三维形变描述理论,设计感应四面体单元微小形变和网格优化的弹性模量、光滑模量和保真模量等度量策略;构建兼顾脑皮层外部形态保持和内部结构优化的最小化调和能量模型及求解算法,优化四面体网格结构;Step 3: Tetrahedral grid optimization: Using the three-dimensional deformation description theory based on the spatial displacement gradient tensor, design measurement strategies for inductive tetrahedral unit micro-deformation and grid optimization such as elastic modulus, smooth modulus, and fidelity modulus ; Construct a minimum harmonic energy model and solution algorithm that takes into account both external shape preservation and internal structure optimization of the cerebral cortex, and optimize the tetrahedral grid structure;

第四步:构建Laplace-Beltramin算子:由定义在黎曼流形M上的调和能量表达式入手, 其中分别表示在黎曼流形M上的网格顶点位置,为定义在网格顶点上的函数表达式;结合四面体单元各表面的矢量表达式,以及体内任意一点的重心坐标表达式,推导以边长和对应两面角变量的四面体顶点之间的几何约束关系;结合三维空间热传导微分方程,在给定的Dirichlet条件(固定脑皮层内、外表面的温度)下,构建Laplace-Beltramin算子的离散表达式;Step 4: Construct the Laplace-Beltramin operator: the harmonic energy expression defined on the Riemannian manifold M start with Respectively represent the grid vertex positions on the Riemannian manifold M, It is a function expression defined on the vertices of the mesh; combining the vector expressions of each surface of the tetrahedron unit and the coordinate expression of the center of gravity of any point in the body, the geometry between the vertices of the tetrahedron with the side length and the corresponding dihedral angle variable is derived Constraint relationship ; Combining with the differential equation of heat conduction in three-dimensional space, under the given Dirichlet condition (fixing the temperature of the inner and outer surfaces of the cerebral cortex), the Laplace-Beltramin operator is constructed The discrete expression of;

第五步:计算脑皮层内部温度场分布:首先构造脑皮层的Dirichlet边界条件;在热平衡条件下定义整个四面体网格为有限求解空间,利用有限元方法求解热传导方程:,其中为Laplace算子,下标M为整个四面体网格空间,是以空间位置和时间为变量的温度函数,将上述偏微分方程转化为线性系统求解脑皮层内部温度场分布;Step 5: Calculating the internal temperature field distribution of the cerebral cortex: first construct the Dirichlet boundary condition of the cerebral cortex; define the entire tetrahedral mesh as a limited solution space under the condition of thermal equilibrium, and use the finite element method to solve the heat conduction equation: ,in is the Laplace operator, the subscript M is the entire tetrahedral grid space, is the spatial position and time As the temperature function of the variable, the above partial differential equation is transformed into a linear system to solve the temperature field distribution inside the cerebral cortex;

第六步:计算脑皮层厚度:通过研究在脑皮层黎曼流形上布朗运动概率密度函数的物理意义,构建由脑皮层局部几何结构所决定的、Laplace-Beltramin算子的特征值和特征向量所表征的热量转移概率表征体系;并计算两个相邻等温层之间,基于最大热量转移概率的热量传导的梯度曲线,最终得到脑皮层内外表面的厚度信息。Step 6: Calculate the thickness of the cerebral cortex: by studying the physical meaning of the Brownian motion probability density function on the Riemannian manifold of the cerebral cortex, construct the eigenvalue and eigenvector representation of the Laplace-Beltramin operator determined by the local geometric structure of the cerebral cortex The heat transfer probability characterization system; and calculate the gradient curve of heat conduction based on the maximum heat transfer probability between two adjacent isothermal layers, and finally obtain the thickness information of the inner and outer surfaces of the cerebral cortex.

该方法能有效地捕捉脑皮层的几何形态变化,能早期对极易转化成AD病症的轻度认知障碍人群(MCI)进行辅助诊断,并根据其演化轨迹揭示其病情发展趋势。This method can effectively capture the geometric changes of the cerebral cortex, and can assist in the early diagnosis of mild cognitive impairment (MCI) who are easily transformed into AD symptoms, and reveal the development trend of the disease according to its evolution trajectory.

附图说明Description of drawings

图1 立方体网格生成结果图,图1(a)为原始球体图像,图1(b)为在保持球体边缘形态的基础上,利用立方体体素填充后的结果。Figure 1. Cube grid generation results. Figure 1(a) is the original sphere image, and Figure 1(b) is the result after filling with cube voxels while maintaining the edge shape of the sphere.

图2 切掉“+”所表示的顶点后在剩余几何体中重构新四面体的三种模板,图中的细线小圆圈代表切面顶点,阴影部分表示切面,“★”、“+”、粗线大圆圈分别表示初始状态下该顶点位于大脑皮层内、外和皮层边缘上。Figure 2 Three templates for reconstructing a new tetrahedron in the remaining geometry after cutting off the vertex indicated by "+". The large circles with thick lines indicate that the vertex is located in the inner, outer and edge of the cerebral cortex in the initial state, respectively.

图3(a)是基于本发明四面体网格生成算法得到的脑皮层图像;图3(b)是脑皮层四面体网格的剖面图,共使用154908个四面体进行填充;图3(c)是生成的四面体网格中所有四面体的二面角分布范围;图3(d)是生成的四面体网格中所有四面体的质量系数分布范围。Fig. 3 (a) is an image of the cerebral cortex obtained based on the tetrahedral mesh generation algorithm of the present invention; Fig. 3 (b) is a cross-sectional view of the tetrahedral mesh of the cerebral cortex, which is filled with 154,908 tetrahedrons; Fig. 3 (c ) is the distribution range of dihedral angles of all tetrahedrons in the generated tetrahedral grid; Figure 3(d) is the distribution range of quality coefficients of all tetrahedrons in the generated tetrahedral grid.

图4 四面体单元示意图。通常在一个四面体单元中,称棱边与棱边和两面角的位置关系是相对的,为棱边的长度。Figure 4 Schematic diagram of tetrahedron unit. Usually in a tetrahedral unit, called edge with edges and dihedral The positional relationship is relative, for the edge length.

图5(a)是合成图像,整体是立方体结构,中间有一个球形的空洞。经过在立方体外表面与球形内表面之间填充四面体之后,形成如图所示的四面体网格结构。图5(b)是在设定外表面温度为1度,内表面为0度时,在达到温度稳定状态下,从四面体网格中切割出的等温面(从左至右,从上至下,分别0.4度—0.9度)。图5(c)是在外表面与内表面之间的温度流场线。图5(d)是根据温度流场线长度得到的从外表面到内表面的厚度信息。Figure 5(a) is a composite image, the whole is a cubic structure with a spherical cavity in the middle. After filling tetrahedrons between the outer surface of the cube and the inner surface of the sphere, a tetrahedral grid structure as shown in the figure is formed. Figure 5(b) is the isothermal surface cut out from the tetrahedral mesh (from left to right, from top to down, respectively 0.4 degrees -0.9 degrees). Figure 5(c) is the temperature flow field lines between the outer surface and the inner surface. Figure 5(d) is the thickness information from the outer surface to the inner surface obtained according to the length of the temperature flow field line.

图6是利用本发明方法和FreeSurfer方法(Fischl, B., Dale, A.M., 2000.Measuring the thickness of the human cerebral cortex from magnetic resonanceimages. Proc. Natl. Acad. Sci. USA 97, 11050-11055.)分别计算的阿尔茨海默病患者(AD)、轻度认知障碍患者(MCI)以及正常人(CTL)三个组别的脑皮层厚度在统计概率下组间的显著性差异影射图。其中,图6(a)、图6(b)分别是本发明方法和FreeSurfer方法得到的AD与CTL组别的显著性差异影射图;图6(c)、图6(d)分别是本发明方法和FreeSurfer方法得到的MCI与CTL组别的显著性差异影射图。在这里,p值越小表示组间的厚度差异性越显著。Fig. 6 is using the method of the present invention and the FreeSurfer method (Fischl, B., Dale, A.M., 2000. Measuring the thickness of the human cerebral cortex from magnetic resonance images. Proc. Natl. Acad. Sci. USA 97, 11050-11055.) The projection map of the significant difference between the three groups of cerebral cortex thickness of Alzheimer's disease patients (AD), mild cognitive impairment patients (MCI) and normal people (CTL) under statistical probability. Among them, Fig. 6(a) and Fig. 6(b) are the significant difference mapping diagrams of AD and CTL groups obtained by the method of the present invention and the FreeSurfer method respectively; Fig. 6(c) and Fig. 6(d) are respectively The mapping map of the significant difference between the MCI and CTL groups obtained by the method and the FreeSurfer method. Here, the smaller the p value, the more significant the difference in thickness between groups.

具体实施方式Detailed ways

本发明的目的是提供一种基于图谱分析理论的脑皮层厚度估计方法,其特征是通过构建脑皮层核磁共振(MRI)图像的四面体网格表征形式和计算调和能量场中的热量传导规律来捕捉MRI脑皮层中的几何信息,具体步骤描述如下:The purpose of the present invention is to provide a method for estimating the thickness of cerebral cortex based on the atlas analysis theory, which is characterized by constructing the tetrahedral grid representation form of the cerebral cortex nuclear magnetic resonance (MRI) image and calculating the heat conduction law in the harmonic energy field. To capture geometric information in the MRI cerebral cortex, the specific steps are described as follows:

第一步:立方体网格生成:首先利用立方体网格填充MRI二值图像,网格顶点的空间属性位置由该点到边缘的距离函数所确定,距离函数的计算采用基于顶点连接关系的快速行进法得到,并标记顶点()所在的正方形为边缘面,通过计算位于边缘上的顶点数目与边缘面所有顶点数目的比值,来自适应调节背景网格边长的大小;例如将一球体利用立方体素单元填充后的结果如图1所示;Step 1: Cube grid generation: Firstly, the cube grid is used to fill the MRI binary image, and the spatial attribute position of the grid vertices is determined by the distance function from the point to the edge As determined, the calculation of the distance function is obtained by the fast marching method based on the connection relationship of vertices, and the vertices are marked ( ) is the edge surface, by calculating the ratio of the number of vertices on the edge to the number of all vertices on the edge surface, the size of the side length of the background grid is adaptively adjusted; for example, the result of filling a sphere with cubic voxel units is shown in the figure 1 shown;

第二步:四面体网格剖分:利用金字塔以及体心立方点阵的形式对边缘面以及内部顶点进行四面体剖分,在此基础上通过四面体每条边两个顶点空间属性的正负校验和线性比例函数对剖分后的四面体网格进行零值面(所有点所连接成的表面)切割与整理,对于某些由于切割造成原四面体结构崩溃的情况,需要通过前期研究工作总结出一些模板来进行新四面体的重建,如图2所示;Step 2: Tetrahedral meshing: Use the form of pyramid and body-centered cubic lattice to divide the edge surface and internal vertices into tetrahedrons. Negative checksum and linear scale function zero-value surface (all of The surface connected by points) is cut and sorted. For some cases where the original tetrahedron structure collapses due to cutting, it is necessary to summarize some templates through the previous research work to reconstruct the new tetrahedron, as shown in Figure 2;

第三步:四面体网格优化:利用包含顶点位移矢量的调和能量函数G(U)最小化微调各顶点的空间位置,其中U=x-XU为位移矢量,x为微调后的坐标向量,X为原始坐标向量,G(U)由惩罚项、光滑项和保真项构成;按照有限应变理论,位移矢量相对于空间坐标系下的偏微分称为空间位移梯度张量,即:,其中,F 称为变形梯度张量,为梯度算子,则格林变形张量为,由C的特征值构成三个描述变形程度的物理量:拉伸量、剪切量以及体积量;在此基础上生成在较大的拓扑形状改动下所产生的拉伸量惩罚、剪切量惩罚以及体积量惩罚项;启动惩罚的阈值条件主要是衡量拉伸量与体积量,剪切量与体积量之间的大小关系,依靠惩罚项保持在每次迭代过程中四面体网格的生成质量;光滑项将每个四面体各顶点位置矢量与位移矢量的差值作为光滑函数的输入,然后通过最小化有限微分的方法,优化区域表面及内部四面体各顶点的位置,消除顶点坐标的起伏;保真项在算法过程中只对边界上的顶点发生作用,即如果迭代后的边界上点偏离原来的体素位置太远,则施加惩罚;调和能量函数的最小化问题采用Sobolev梯度算法进行求解,最终生成保持MRI影像数据边界拓扑形状与整体光滑稳健的四面体网格;图3为利用本文四面体网格生成算法得到的脑皮层网格图像,从图3可见,由于实施了网格边缘保持与结构优化策略,保证了网格符合原有图像的精细的拓扑结构,同时提升了网格中每个四面体的生成质量,为后续Laplace-Beltramin算子等数值计算提供了精确度的保证;The third step: Tetrahedral grid optimization: use the harmonic energy function G ( U ) containing the vertex displacement vector to minimize the spatial position of each vertex, where U=xX , U is the displacement vector, x is the coordinate vector after fine-tuning, X is the original coordinate vector, G ( U ) is composed of penalty term, smooth term and fidelity term; according to the finite strain theory, the partial differential of the displacement vector relative to the spatial coordinate system is called the spatial displacement gradient tensor, namely: , where F is called the deformation gradient tensor, is the gradient operator, then the Green deformation tensor is , the eigenvalues of C form three physical quantities describing the degree of deformation: stretching amount, shearing amount, and volume; on this basis, the stretching amount penalty and shearing amount generated under large topological shape changes are generated Penalty and volume penalty item; the threshold condition for starting the penalty is mainly to measure the relationship between the stretching amount and the volume amount, the shear amount and the volume amount, and rely on the penalty item to maintain the generation of the tetrahedral mesh during each iteration Quality; the smooth item uses the difference between the position vector and the displacement vector of each tetrahedron as the input of the smooth function, and then optimizes the position of each vertex on the surface of the area and the internal tetrahedron by minimizing the finite differential method, eliminating the vertex coordinates Ups and downs; the fidelity item only acts on the vertices on the boundary during the algorithm process, that is, if the point on the boundary after iteration deviates too far from the original voxel position, a penalty will be imposed; the minimization of the harmonic energy function uses the Sobolev gradient algorithm Finally, a tetrahedral grid that maintains the topological shape of the boundary of the MRI image data and the overall smoothness and stability is generated; Figure 3 shows the grid image of the cerebral cortex obtained by using the tetrahedral grid generation algorithm in this paper. It can be seen from Figure 3 that due to the implementation of the network The grid edge preservation and structure optimization strategy ensures that the grid conforms to the fine topology of the original image, and at the same time improves the generation quality of each tetrahedron in the grid, providing accuracy for subsequent numerical calculations such as Laplace-Beltramin operators guarantee;

第四步:构建Laplace-Beltramin算子:将生成的四面体网格定义为含有内部和边缘顶点的有限求解区域,然后按照公式(1)计算四面体网格的局部刚性矩阵Step 4: Construct the Laplace-Beltramin operator: define the generated tetrahedral mesh as a limited solution area containing internal and edge vertices, and then calculate the local rigidity matrix of the tetrahedral mesh according to formula (1) :

(1) (1)

其中,为四面体网格中的顶点序号,为离散调和能量因子,其计算方法如下:在特定的四面体网格中,假设棱边被n个四面体所公用,则在每个四面体中,棱边所相对的棱边和两面角,分别记为,如图4所示,那么在所有n个四面体中,棱边所相对的所有棱边和两面角可记为,则in, is the vertex number in the tetrahedral mesh, is the discrete harmonic energy factor, and its calculation method is as follows: In a specific tetrahedral grid, assuming that the edge is shared by n tetrahedrons, then in each tetrahedron, the edge The opposite edges and dihedral angles are denoted as and , as shown in Figure 4, then in all n tetrahedrons, the edge All the opposite edges and dihedral angles can be written as ,but

(2) (2)

最后,利用公式(3)得到Dirichlet边界条件下的Laplace-Beltramin算子:Finally, use the formula (3) to get the Laplace-Beltramin operator under the Dirichlet boundary condition:

(3) (3)

其中,D为对角矩阵,定义为where D is a diagonal matrix defined as ;

第五步:计算脑皮层内部温度场分布:首先将脑皮层外表面各顶点的温度赋值为1,内表面各顶点的温度赋值为0,以此来构造脑皮层的Dirichlet边界条件;通过公式(3)得到的Laplace-Beltramin算子作为求解在脑皮层内部调和能量场中热量稳定扩散分布的功能算子;利用下列公式求解脑皮层内部温度场分布:Step 5: Calculating the internal temperature field distribution of the cerebral cortex: first assign the temperature of each vertex on the outer surface of the cerebral cortex to 1, and assign the temperature of each vertex on the inner surface to 0, so as to construct the Dirichlet boundary condition of the cerebral cortex; through the formula ( 3) The obtained Laplace-Beltramin operator As a functional operator to solve the stable diffusion distribution of heat in the harmonic energy field inside the cortex; use the following formula to solve the temperature field distribution inside the cortex:

(4) (4)

其中,的向量,表示n个脑皮层内表面顶点,的向量,表示m个脑皮层内、外表面的顶点;例如在合成图像5(a)中,利用公式(4)求解内外表面间的温度场后,从四面体网格中切割出的各个等温面;in, Yes A vector representing n vertices on the inner surface of the cortex, Yes The vector of m represents the vertices of the inner and outer surfaces of the cerebral cortex; for example, in the composite image 5(a), after solving the temperature field between the inner and outer surfaces using formula (4), each isotherm cut out from the tetrahedral mesh noodle;

第六步:计算脑皮层厚度:首先按照图谱分析理论,构建热核扩散因子:Step 6: Calculating the thickness of the cerebral cortex: First, according to the map analysis theory, construct the thermonuclear diffusion factor:

(5) (5)

其中,分别表示Laplace-Beltramin算子的第i个特征值和特征向量,表示在传导时间t内单位热量由x沿传播路径到y的概率密度函数,其最大的概率密度传播路径即为热量传播的梯度方向;然后根据第五步得到的等温层,从脑皮层外表面的一个顶点x出发,利用公式(5)计算从x到下一个等温层各点的热量传播概率密度,搜索最大的概率密度所对应的下一个等温层的y点,连接x和y即为这两个相邻等温层的热量传播梯度方向;然后再以y为起点,搜索下一个等温层的最大热量概率密度传播路径,以此类推,直到内表面为止,连接所有等温层之间的最大热量概率密度传播路径,即可得到从脑皮层外表面一点到内表面的局部厚度值,遍历外表面所有顶点,利用第六步计算方法,可获得脑皮层的全局厚度值。图5(c)是利用图谱分析理论,按照最大热量概率密度计算得到的热量传播梯度曲线;图5(d)是根据外表面到内表面的温度流场线长度映射到外表面的厚度信息。in, and represent the i-th eigenvalue and eigenvector of the Laplace-Beltramin operator, respectively, Indicates the probability density function of unit heat from x along the propagation path to y within the conduction time t, and its maximum probability density propagation path is the gradient direction of heat propagation; then according to the isothermal layer obtained in the fifth step, from the outer surface of the cerebral cortex Starting from a vertex x of , use the formula (5) to calculate the heat transfer probability density from x to each point in the next isothermal layer , search for the y point of the next isothermal layer corresponding to the maximum probability density, connect x and y is the heat propagation gradient direction of the two adjacent isothermal layers; then start from y, search for the maximum Heat probability density propagation path, and so on, until the inner surface, connect the maximum heat probability density propagation path between all isothermal layers, you can get the local thickness value from a point on the outer surface of the cerebral cortex to the inner surface, traverse all the outer surface At the vertex, the global thickness value of the cerebral cortex can be obtained by using the calculation method in the sixth step. Figure 5(c) is the heat transfer gradient curve calculated according to the maximum heat probability density using the map analysis theory; Figure 5(d) is the thickness information mapped to the outer surface according to the length of the temperature flow field line from the outer surface to the inner surface.

Claims (1)

1. A method for estimating the thickness of a cerebral cortex based on a spectrum analysis theory is characterized in that geometric information in the cerebral cortex of a brain cortex Magnetic Resonance (MRI) is captured by constructing a tetrahedral mesh representation form of the MRI image of the cerebral cortex and calculating a heat conduction rule in a harmonic energy field, and the specific steps are described as follows:
the first step is as follows: and (3) generating a cubic grid: generating a background grid consisting of cubic units on the basis of keeping the shape of the boundary; calculating the spatial position attribute of the grid point of the background cube with the symbolic feature by adopting a fast marching method based on the vertex connection relation, and designing an operation rule for adaptively adjusting the side length of the grid through the probability distribution of the spatial position of the grid point near the edge surface so as to achieve the optimal degree of fitting the cerebral cortex;
a second step of tetrahedral mesh division, which is to respectively perform tetrahedral division on the background meshes at the edge surface and the internal vertex by adopting a pyramid division form and a body-centered cubic lattice division form, and then perform zero surface cutting and finishing on the divided tetrahedral meshes;
the third step: and (3) tetrahedral mesh optimization: designing measurement strategies such as elastic modulus, smooth modulus, fidelity modulus and the like for sensing the micro deformation of the tetrahedral unit and optimizing the grid by using a three-dimensional deformation description theory based on the spatial displacement gradient tensor; constructing a minimum harmonic energy model and a solving algorithm which take account of the preservation of the external morphology of the cerebral cortex and the optimization of the internal structure, and optimizing a tetrahedral mesh structure;
the fourth step: constructing a Laplace-Beltramin operator: by expression of harmonic energy defined on Riemannian manifold MTo start with, whereinRespectively representing the mesh vertex positions on the riemann manifold M,is a function expression defined on the mesh vertex; combining vector expressions of all surfaces of the tetrahedron units and barycentric coordinate expressions of any point in the body, and deducing a geometric constraint relation between tetrahedron vertexes with side length and corresponding two-side angle variables(ii) a Combining a three-dimensional space heat conduction differential equation, and constructing a Laplace-Beltramin operator under a given Dirichlet condition (temperature of the inner surface and the outer surface of a fixed cerebral cortex)The discrete expression of (a);
the fifth step: calculating the internal temperature field distribution of the cerebral cortex: firstly, constructing Dirichlet boundary conditions of a cerebral cortex; defining the whole tetrahedral mesh as a finite solution space under the condition of thermal balance, and solving a heat conduction equation by using a finite element method:whereinAs Laplace operator, subscriptMIs the whole tetrahedral mesh space and is a tetrahedral mesh,is in spatial positionAnd timeConverting the partial differential equation into a linear system to solve the temperature field distribution in the cerebral cortex as a temperature function of a variable;
and a sixth step: calculating the thickness of the cerebral cortex: constructing a heat transfer probability characterization system which is determined by a local geometric structure of the cerebral cortex and is characterized by a characteristic value and a characteristic vector of a Laplace-Beltramin operator by researching the physical significance of a Brownian motion probability density function on the riemann manifold of the cerebral cortex; and calculating a gradient curve of heat conduction between two adjacent isothermal layers based on the maximum heat transfer probability.
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