低计数率光子计数探测器数值无偏衰减路径长度估计器的存在性、唯一性和效率

IF 3.2 2区 医学 Q1 RADIOLOGY, NUCLEAR MEDICINE & MEDICAL IMAGING
Medical physics Pub Date : 2024-09-17 DOI:10.1002/mp.17406
Scott S. Hsieh, Paurakh L. Rajbhandary
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引用次数: 0

摘要

背景计算机断层扫描(CT)重建的第一步是估计衰减路径长度。通常采用对数变换,这是比尔-朗伯定律的直接解决方案。然而,在低信号时,对数估计器会出现偏差。偏差既来自对数的曲率,也来自检测到零计数的可能性,因此可以采用数据替换策略来避免对数的奇异性。最近,Li 等人[IEEE Trans Med Img 42:6, 2023]在修改对数估计器以消除曲率偏差方面取得了进展,但减轻奇异性偏差的最佳策略仍然未知。目的本研究的目的是利用数值技术构建无偏衰减路径长度估计器,作为对数估计器的替代方案,并研究可能解决方案的唯一性和最优性,假设探测器为光子计数探测器。方法通常,衰减路径长度估计器是从整数探测器计数到实际路径长度值的映射。我们只关注对数估计器有问题的小信号输入(我们将其定义为 100 计数的输入),并考虑仅使用单个输入且不受相邻测量影响的估计器(如自适应平滑)。所有可能的路径长度估计器集合都可以用 100 维向量空间中的点来表示。在这个向量空间中,我们通过优化来选择 (1) 均方误差最小和 (2) 无偏的估计器。我们将 "无偏 "定义为满足数值条件,即最大偏差小于 0.001,横跨所需的操作范围内 1000 个物体厚度的连续体。由于目标函数是凸函数,而约束条件是仿射的,因此优化是可控的,并能保证收敛到全局最小值。我们进一步研究了约束矩阵的无效空间,以了解可能解的唯一性,并将结果与方差的克拉梅尔-拉奥约束进行了比较。结果我们首先证明,如果允许非常低的平均探测器信号(等同于非常厚的物体),则不存在无偏衰减路径长度估计器。有必要选择一个最小的平均检测器信号,以实现无偏行为。如果我们选择两个计数,最佳估计器与李的估计器相似。如果我们选择一个计数,最优估计器就会变成非单调估计器。振荡会导致无偏估计器的噪声放大。约束矩阵的无效空间是高维的,因此无偏解不是唯一的。结论如果允许任意厚度的物体,则不存在无偏衰减路径长度估计器。如果限制最大厚度,则存在无偏估计器,但并非唯一。可以选择方差最小的最优估计器,但存在偏差与方差的权衡,即更大的无偏域需要更大的方差。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Existence, uniqueness, and efficiency of numerically unbiased attenuation pathlength estimators for photon counting detectors at low count rates
BackgroundThe first step in computed tomography (CT) reconstruction is to estimate attenuation pathlength. Usually, this is done with a logarithm transformation, which is the direct solution to the Beer‐Lambert Law. At low signals, however, the logarithm estimator is biased. Bias arises both from the curvature of the logarithm and from the possibility of detecting zero counts, so a data substitution strategy may be employed to avoid the singularity of the logarithm. Recent progress has been made by Li et al. [IEEE Trans Med Img 42:6, 2023] to modify the logarithm estimator to eliminate curvature bias, but the optimal strategy for mitigating bias from the singularity remains unknown.PurposeThe purpose of this study was to use numerical techniques to construct unbiased attenuation pathlength estimators that are alternatives to the logarithm estimator, and to study the uniqueness and optimality of possible solutions, assuming a photon counting detector.MethodsFormally, an attenuation pathlength estimator is a mapping from integer detector counts to real pathlength values. We constrain our focus to only the small signal inputs that are problematic for the logarithm estimator, which we define as inputs of <100 counts, and we consider estimators that use only a single input and that are not informed by adjacent measurements (e.g., adaptive smoothing). The set of all possible pathlength estimators can then be represented as points in a 100‐dimensional vector space. Within this vector space, we use optimization to select the estimator that (1) minimizes mean squared error and (2) is unbiased. We define “unbiased” as satisfying the numerical condition that the maximum bias be less than 0.001 across a continuum of 1000 object thicknesses that span the desired operating range. Because the objective function is convex and the constraints are affine, optimization is tractable and guaranteed to converge to the global minimum. We further examine the nullspace of the constraint matrix to understand the uniqueness of possible solutions, and we compare the results to the Cramér‐Rao bound of the variance.ResultsWe first show that an unbiased attenuation pathlength estimator does not exist if very low mean detector signals (equivalently, very thick objects) are permitted. It is necessary to select a minimum mean detector signal for which unbiased behavior is desired. If we select two counts, the optimal estimator is similar to Li's estimator. If we select one count, the optimal estimator becomes non‐monotonic. The oscillations cause the unbiased estimator to be noise amplifying. The nullspace of the constraint matrix is high‐dimensional, so that unbiased solutions are not unique. The Cramér‐Rao bound of the variance matches well with the expected scaling law and cannot be attained.ConclusionIf arbitrarily thick objects are permitted, an unbiased attenuation pathlength estimator does not exist. If the maximum thickness is restricted, an unbiased estimator exists but is not unique. An optimal estimator can be selected that minimizes variance, but a bias‐variance tradeoff exists where a larger domain of unbiased behavior requires increased variance.
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来源期刊
Medical physics
Medical physics 医学-核医学
CiteScore
6.80
自引率
15.80%
发文量
660
审稿时长
1.7 months
期刊介绍: Medical Physics publishes original, high impact physics, imaging science, and engineering research that advances patient diagnosis and therapy through contributions in 1) Basic science developments with high potential for clinical translation 2) Clinical applications of cutting edge engineering and physics innovations 3) Broadly applicable and innovative clinical physics developments Medical Physics is a journal of global scope and reach. By publishing in Medical Physics your research will reach an international, multidisciplinary audience including practicing medical physicists as well as physics- and engineering based translational scientists. We work closely with authors of promising articles to improve their quality.
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