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Assessment of the effects of scatterer size distributions on effective scatterer diameter estimates

机译:评估散射体尺寸分布对有效散射体直径估计值的影响

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Scattering models used in most quantitative ultrasound studies assume distributions of identical scatterers. However, actual tissues may exhibit multiple levels of spatial scales. Therefore, the objective of the present study was to use both simulations and experiments to analyze the effects of scatterer size distributions when using a fluid-sphere model for estimating effective scatterer diameter (ESD). Simulations were conducted with populations of scatterers with uniformly distributed sizes within [25, 100], [25, 50], [50, 100], and [50, 75] μm. Simulated backscatter coefficients (BSCs) used as inputs for the ESD estimator were obtained using two methods: (1) using portions of the theoretical BSC with different center frequencies between 1 and 40 MHz and 100% fractional bandwidth, and (2) processing simulated radiofrequency data from computer phantoms using f/4 transducers with center frequencies of 3, 6, 12, 24, and 36 MHz and 100% fractional bandwidth. Experiments were conducted using a gelatin phantom with Sephadex spheres ranging in diameter from 30 μm to 140 μm and 3.5, 7.5, 10, and 13 MHz focused transducers. ESD estimates obtained with both simulation methods were approximately inversely proportional to frequency and mostly independent of the underlying scatterer size distribution for sufficiently high analysis frequencies. For frequencies higher than 13 MHz the ESD estimates were below 50 μm for all considered size distributions even though two of them had no scatterers smaller than 50 μm. Further, the asymptotic behavior of ESD vs. frequency estimates was also observed experimentally. The results of this work highlight some of the effects of continuous scatterer size distributions when obtaining ESD estimates, and challenge the hypothesis that different frequency ranges are more sensitive to different spatial scales when using a single-size scattering model. Although the results presented here are not necessarily u--niversal and most likely will be affected by the actual size distribution and frequency-dependent BSC of the individual scatterers, this work suggests that caution must be exerted when interpreting ESD estimates at different frequency ranges. This work was supported by a grant from the NIH R21CA139095.
机译:大多数定量超声研究中使用的散射模型均假设相同散射体的分布。但是,实际组织可能会表现出多个级别的空间尺度。因此,本研究的目的是在使用流体球体模型估算有效散射体直径(ESD)时,同时使用仿真和实验来分析散射体尺寸分布的影响。对散射体进行了模拟,这些散射体的大小均匀分布在[25,100],[25,50],[50,100]和[50,75]μm之内。使用两种方法获得了用作ESD估计器输入的模拟反向散射系数(BSC):( 1)使用理论BSC的部分中心频率在1和40 MHz之间且分数带宽为100%的部分,以及(2)处理模拟射频使用中心频率分别为3、6、12、24和36 MHz的f / 4传感器和100%的分数带宽从计算机幻象中获取数据。使用明胶体模和Sephadex球体进行实验,球体的直径范围为30μm至140μm,并使用3.5、7.5、10和13 MHz聚焦换能器。通过两种仿真方法获得的ESD估计值与频率近似成反比,并且对于独立于足够高的分析频率的散射器大小分布,大多与之无关。对于高于13 MHz的频率,所有考虑的尺寸分布的ESD估计值均低于50μm,即使其中两个没有小于50μm的散射。此外,还通过实验观察到ESD与频率估计值的渐近行为。这项工作的结果突出了获得ESD估计值时连续散射体尺寸分布的一些影响,并挑战了使用单一尺寸散射模型时不同频率范围对不同空间比例更敏感的假设。尽管此处显示的结果不一定是u- -- 单个散射体的实际大小分布和与频率相关的BSC可能会影响整个范围,因此这项工作表明,在解释不同频率范围的ESD估计值时必须格外小心。这项工作得到了NIH R21CA139095的资助。

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