基于稀疏多模分散Radon变换的波导参数实时估计

Claudio Araya, Alejandro Martinez, D. Ramiandrisoa, Dean Ta, Kailiang Xu, A. Osses, J. Minonzio
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引用次数: 1

摘要

骨质疏松和相关的脆性骨折仍然是一个社会问题。已经提出了几种定量超声方法来克服当前金标准DXA的局限性。双向轴向传输(BDAT)是基于测量由骨皮质壳引导的波。皮质厚度(Ct.Th)和孔隙度(Ct.Po)估计值对应于目标函数Proj(Ct.Th,Ct.Po)的最大值,最初定义为被测模型在奇异向量基(方法1)中的投影。每个模型矩阵具有相同的维度,即Nf=124 x Nk=256, 512, 1024或2048像素,超声导波光谱实验图像Norm(f,k)。模型总数等于n,=38 x Npo=25,即考虑皮质厚度和孔隙率的数量,范围分别为0.8 ~ 4.5 mm和1 ~ 25%。最后,备选目标函数(NthxNpo像素)的每个像素对应于一个模型与实验导波频谱图像之间的逐像素图像乘法(方法2)或实验与模型重构向量之间的稀疏矩阵乘法(方法3)。这三种方法在400次测量数据上进行了测试。观察到方法2和方法3提供相同的Ct。Ct。与方法1的差异随Nk的增加而减小。可接受的差异,即低于典型的测量分辨率(0.2 mm的Ct)。Nk=2048时,Ct.Po为1%。在标准桌面上使用Matlab,方法1和方法3的计算时间分别为20秒、4秒和0.3秒。方法3用c++在5ms内完成计算。最后一个值打开了使用实时目标函数指导界面改进的视角。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Real Time Waveguide Parameter Estimation Using Sparse Multimode Disperse Radon Transform
Osteoporosis and associated fragility fractures are still a societal problem. Several quantitative ultrasound approaches have been proposed to overcome limitations of the current gold standard DXA. Bi Directional Axial Transmission (BDAT) is based on the measurement of waves guided by the cortical bone shell. Cortical thickness (Ct.Th) and porosity (Ct.Po) estimates correspond to the maxima of the objective function Proj(Ct.Th,Ct.Po), initially defined as the projection of a tested model in the singular vector basis (method 1). Each model matrix has the same dimension, i.e., Nf=124 x Nk=256, 512, 1024 or 2048 pixels, of an ultrasonic guided wave spectrum experimental image Norm(f,k). The total number of models is equal to Nth,=38 x Npo=25, i.e., the number of cortical thickness and porosity taken into account, ranging respectively from 0.8 to 4.5 mm and 1 to 25%. Finally, each pixel of the alternative objective function (NthxNpo pixels) corresponds to the pixel-wise image multiplication between one model and the experimental guided wave spectrum image (method 2) or a sparse matrix multiplication between experimental and model reshaped vectors (method 3). The three methods were tested on data obtained on 400 measurements. It was observed that methods 2 and 3 provided the same Ct.Th Ct.Po values while differences with method 1 decreased with Nk. Acceptable differences, i.e., lower than the typical measurement resolution (0.2 mm for Ct.Th and 1% for Ct.Po) were achieved for Nk=2048. Using Matlab on a standard desktop, this calculation took 20, 4 and 0.3 s, for the methods 1 to 3, respectively. Method 3 calculation was achieved in 5 ms using C++. This last value opens perspective toward guiding interface improvement using real time objective function.
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