Optimizing energy threshold selection for low-concentration contrast agent quantification in small animal photon-counting CT.

IF 3.3 3区 医学 Q2 ENGINEERING, BIOMEDICAL
Xiaoyu Hu, Yuncheng Zhong, Xun Jia, Kai Yang
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引用次数: 0

Abstract

Objective.Gold nanoparticles (GNPs) are widely used for biological research and applications. The in-vivo concentration of GNPs is usually low due to biological safety concerns, thus posing a challenge for imaging. This work investigates on optimal energy threshold selection in photon-counting detector(PCD)-based CT (PCCT) for the quantification of low-concentration GNPs.Approach.We derived the mathematical expression of the upper bound of the material decomposition error in the gold image. Comprehensive simulations were implemented for cylindrical phantom with inserts of different GNP concentrations. CT scans of this phantom were simulated with a 140 kVp x-ray beam under a realistic pre-clinical CT dose range. The PCD energy thresholds from 30 to 110 keV were enumerated for 2,3-channel PCCT and the optimal energy thresholds were determined by searching for the lowest decomposition error.Main results.The optimal energy threshold(s) to minimize the decomposition error in gold image was 44 keV for the 2-channel PCCT and{34,40}keV for the 3-channel case. Numerical results also validated the derived upper bounds of the decomposition error.Significance.This work addressed the need for selecting appropriate energy thresholds for accurate quantification of contrast agent distributions in pre-clinical PCCT. Both the analytical expression of the upper bound of material decomposition error and simulation results showed that the balanced consideration on photon counting noise levels and the numerical properties of the decomposition matrix is required in selecting the appropriate energy thresholds to achieve the most accurate material decomposition.

优化小动物光子计数CT低浓度造影剂定量的能量阈值选择。
目的:纳米金在生物学研究中有着广泛的应用前景。由于生物安全考虑,GNPs的体内浓度通常较低,因此对成像构成挑战。本文研究了基于光子计数检测器(PCD)的CT (PCCT)中用于定量低浓度GNPs的最佳能量阈值选择。& # xD;方法。导出了金图像中材料分解误差上界的数学表达式。对插入不同GNPs浓度的圆柱形体进行了综合仿真。在真实的临床前CT剂量范围内,用140 kVp x射线束模拟该幻影的CT扫描。对2、3通道PCCT列举了30 ~ 110 keV的PCD能量阈值,通过寻找分解误差最小的方法确定了最佳能量阈值。& # xD;主要结果。对于2通道PCCT,最小化金色图像分解误差的最佳能量阈值为44 keV,对于3通道PCCT,则为{34,40}keV。数值结果也验证了所导出的分解误差上界。& # xD;意义。这项工作解决了在临床前PCCT中选择合适的能量阈值以准确量化造影剂分布的需要。材料分解误差上界的解析表达式和仿真结果都表明,在选择合适的能量阈值时,需要平衡考虑光子计数噪声级和分解矩阵的数值性质,以实现最精确的材料分解。& # xD。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Physics in medicine and biology
Physics in medicine and biology 医学-工程:生物医学
CiteScore
6.50
自引率
14.30%
发文量
409
审稿时长
2 months
期刊介绍: The development and application of theoretical, computational and experimental physics to medicine, physiology and biology. Topics covered are: therapy physics (including ionizing and non-ionizing radiation); biomedical imaging (e.g. x-ray, magnetic resonance, ultrasound, optical and nuclear imaging); image-guided interventions; image reconstruction and analysis (including kinetic modelling); artificial intelligence in biomedical physics and analysis; nanoparticles in imaging and therapy; radiobiology; radiation protection and patient dose monitoring; radiation dosimetry
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