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Scatterer size estimation in pulse-echo ultrasound using focused sources: Theoretical approximations and simulation analysis

机译:使用聚焦源估算脉冲回波超声中的散射体尺寸:理论近似和仿真分析

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摘要

The speckle in ultrasound images has long been thought to contain information related to the tissue microstructure. Many different investigators have analyzed the frequency characteristics of the backscattered signals to estimate the scatterer acoustic concentration and size. Previous work has been mostly restricted to unfocused or weakly focused ultrasound sources, thus limiting its implementation with diagnostically relevant fields. Herein, we derive equations capable of estimating the size of a scatterer for any reasonably focused source provided that the velocity potential field in the focal region can be approximated as a three-dimensional Gaussian beam, scatterers are a sufficient distance from the source, and the field is approximately constant across the scatterer. The calculations show that, when estimating the scatterer size, correcting for focusing requires a generalized attenuation-compensation function that includes both attenuation and focusing along the beam axis. The Gaussian approximation is validated by comparing the ideal velocity potential field for three spherically focused sources with f-numbers of 1, 2, and 4 to the Gaussian approximation for frequencies from 2 to 14 MHz. The theoretical derivations are evaluated by simulating the backscatter by using spherically focused sources (f-numbers of 1, 2, and 4) adjacent to attenuating media (0.05 to 1 dB/cm/MHz) that contain scatterers with Gaussian impedance distributions. The generalized attenuation-compensation function yielded results accurate to 7.2% while the traditional attenuation-compensation functions that neglected focusing had errors as high as 103%.
机译:长期以来,超声图像中的斑点一直被认为包含与组织微结构有关的信息。许多不同的研究人员已经分析了反向散射信号的频率特性,以估计散射体的声波浓度和大小。先前的工作主要限于未聚焦或聚焦较弱的超声源,因此将其在诊断相关领域的实施受到了限制。在此,我们推导出能够估算任何合理聚焦源的散射体大小的方程式,条件是焦点区域中的速度势场可以近似为三维高斯光束,散射体与源之间的距离足够远,并且场在散射体上近似恒定。计算表明,在估计散射体尺寸时,校正聚焦需要通用的衰减补偿功能,该功能包括沿光束轴的衰减和聚焦。高斯近似值通过比较f值为1、2和4的三个球形聚焦源的理想速度势场与2至14 MHz频率的高斯近似值进行验证。通过使用与包含高斯阻抗分布的散射体的衰减介质(0.05到1 dB / cm / MHz)相邻的球形聚焦源(f值为1、2和4)模拟反向散射,可以评估理论推导。广义的衰减补偿函数产生的结果精确到7.2%,而传统的忽略聚焦的衰减补偿函数的误差高达103%。

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