利用最大空间滞后一相干度量灵活估计阵列曲率和声速

Jiaxin Zhang, Kai Ding, M. L. Lediju Bell
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摘要

柔性换能器阵列有可能在光声图像引导介入过程中适应各种器官的形状和大小。然而,不正确的声速和阵列形状会干扰光声目标定位并降低图像质量。我们提出了一种估算目标周围声速和近似凹形柔性阵列曲率半径的指标。该指标被定义为从光声目标周围感兴趣区域接收到的时延零均值信道数据的最大滞后一空间一致性(我们简称为 mLOC)。我们用模拟和实验幻影数据证明了其性能。在中等声速为 1540 米/秒的 k 波中模拟了三个光声目标,光声信号由一个形状扁平、曲率半径为 81.3 毫米的传感器接收。为了获取放置在平面和曲面上的柔性阵列的光声实验数据,将光纤与空心金属针配对插入半径为 83 毫米的半球形塑料溶胶模型的三个位置。在采用波束成形时间延迟计算 mLOC 时,相关声速和曲率半径分别为 1080-2000 米/秒和 60-120 毫米。在模拟中,通过最大化 mLOC 估算的声速和阵列曲率分别为 1540 米/秒和 81 毫米,精确度分别为 100%和 99.63%。根据 mLOC 最大值的经验估算,幻影中的声速为 1543 m/s,由此估算出的阵列曲率为 85 mm,相应的准确率为 97.59%。结果表明,当声速和阵列半径这些变量在未来柔性阵列成像方案中未知时,mLOC 具有近似这些变量的潜力。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flexible array curvature and sound speed estimations with a maximum spatial lag-one coherence metric
Flexible transducer arrays have the potential to conform to various organ shapes and sizes during photoacoustic image-guided interventions. However, incorrect sound speeds and array shapes can interfere with photoacoustic target localization and degrade image quality. We propose a metric to estimate the sound speed surrounding a target and the radii of curvature of flexible arrays with approximately concave shapes. The metric is defined as the maximum lag-one spatial coherence of the time-delayed, zero-mean channel data received from a region of interest surrounding a photoacoustic target (which we abbreviate as mLOC). Performance is demonstrated with simulated and experimental phantom data. Three photoacoustic targets were simulated in k-Wave with 1540 m/s medium sound speed, and photoacoustic signals were received by a transducer with a flat shape and an 81.3 mm radius of curvature. To acquire experimental photoacoustic data with the flexible array placed on flat and curved surfaces, an optical fiber paired with a hollow metal needle was inserted into an 83-mm-radius hemispherical plastisol phantom at three locations. When implementing beamforming time delays to calculate mLOC, the associated sound speed and radii of curvature ranged 1080-2000 m/s and 60-120 mm, respectively. The sound speed and array curvature estimated by the maximized mLOC were 1540 m/s and 81 mm, respectively, in simulation, resulting in accuracies of 100% and 99.63%, respectively. The sound speed in the phantom was empirically estimated by the maximum of mLOC as 1543 m/s, which led to the array curvature estimation of 85 mm and the corresponding accuracy of 97.59%. Results demonstrate the potential of mLOC to approximate sound speeds and array radii when these variables are unknown in future flexible array imaging scenarios
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