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The impact of different estimator algorithms when obtaining effective diameter estimates from populations of scatterers of different sizes

机译:从不同尺寸的散射体中获得有效直径估算值时,不同估算器算法的影响

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Quantitative ultrasound using backscatter coefficients (BSCs) is a potentially powerful tool for estimating microstructural properties from tissues. However, most scattering models assume distributions of identical scatterers even though actual tissues exhibit different levels of spatial variations. It has been experimentally demonstrated that the use of single-size scattering models may yield effective scatterer diameter (ESD) estimates that are not physically meaningful, i.e., estimates that do not correspond to the size of actual physical structures present in the analysis medium. The objective of this study is to analyze three different estimator algorithms when estimating ESDs from media with populations of fluid-like spherical scatterers of different sizes. All estimator algorithms used a single-sized fluid sphere scattering model for ESD estimation. The estimators corresponded to minimizing (1) the variance of the ratio in decibels between the estimated BSCs and the scattering model, (2) the root mean square error (RMSE) between the estimated BSC and a scaled version of the scattering model, and (3) the RMSE between the estimated BSC and a linear transformation (allowing for an intercept) of the scattering model. In simulations, the inputs to the ESD estimators were obtained using portions of the theoretical BSC (neglecting multiple scattering and coherent scattering terms) with different center frequencies between 1 and 40 MHz and 100% fractional bandwidth corresponding to several scatterer size distributions ranging between 25 and 100 µm. In experiments, BSCs were estimated from a gelatin phantom with Sephadex spheres ranging in diameter from 70 to 130 µm and 5-, 7.5-, 10-, and 13-MHz focused transducers. In simulations, ESD estimates obtained with Estimator 1 were approximately inversely proportional to frequency and mostly independent of the underlying scatterer size distribution for sufficiently large analysis frequencies. Estimator 2 al- o converged to physically meaningless solutions for sufficiently large frequencies, but generally allowed convergence for higher frequencies than Estimator 1. Estimator 3, in contrast, produced meaningful estimates for all studied analysis frequencies and all simulated media. In experiments, Estimator 1 produced ESD estimates lower than 70 µm when using both the 10- and 13-MHz data. However, Estimators 2 and 3 produced ESD estimates between 80 and 100 µm from the same experimental BSCs. The results of this work demonstrate that ESD estimates are highly dependent on the algorithm used to produce them. Results from both simulations and experiments suggest that single-size scattering models may produce meaningful ESD estimates for moderately large ka factors with the use of a proper estimator algorithm.
机译:使用背向散射系数(BSC)的定量超声是从组织估计微结构特性的潜在强大工具。但是,即使实际组织显示出不同水平的空间变化,大多数散射模型仍假定散射体的分布相同。实验已经证明,使用单一尺寸的散射模型可能会产生在物理上没有意义的有效散射体直径(ESD)估算值,即与分析介质中实际物理结构的尺寸不符的估算值。这项研究的目的是在估计具有不同大小的类流体球形散射体的介质中的ESD时,分析三种不同的估计器算法。所有估算器算法均使用单一尺寸的流体球体散射模型进行ESD估算。估计量对应于使(1)估计的BSC与散射模型之间的分贝比率的方差最小化;(2)估计的BSC与散射模型的缩放版本之间的均方根误差(RMSE),以及( 3)估计的BSC与散射模型的线性变换(允许截距)之间的RMSE。在仿真中,使用理论BSC的一部分(忽略多个散射和相干散射项)获得ESD估算器的输入,这些BSC的中心频率在1至40 MHz之间,并且分数带宽为100%,对应于25至50之间的几个散射体尺寸分布100微米在实验中,BSC是从明胶模型中估计的,其中的Sephadex球的直径范围为70至130 µm,并带有5、7.5、10、13 MHz聚焦换能器。在仿真中,用估计器1获得的ESD估计值与频率近似成反比,并且对于足够大的分析频率而言,基本上与下面的散射体大小分布无关。估计器2还可以收敛到足够大的频率而对物理上毫无意义的解,但是通常允许比估计器1更高的频率收敛。估计器3相反地为所有研究的分析频率和所有模拟媒体提供了有意义的估计。在实验中,当同时使用10 MHz和13 MHz数据时,估计器1产生的ESD估计值低于70 µm。但是,估计器2和3根据相同的实验BSC得出80至100 µm的ESD估计值。这项工作的结果表明,ESD估计高度依赖于用于产生它们的算法。来自仿真和实验的结果均表明,使用适当的估算器算法,单一尺寸的散射模型可能会对中等大的ka因子产生有意义的ESD估算值。

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