Hu Xiaoyu, Zhong Yuncheng, Jia Xun, Yang Kai
Department of Radiation Oncology and Molecular Radiation Sciences, Johns Hopkins University, Baltimore, MD, United States of America.
Division of Diagnostic Imaging Physics, Department of Radiology, Massachusetts General Hospital, Boston, MA, United States of America.
Phys Med Biol. 2025 Feb 3;70(4). doi: 10.1088/1361-6560/adac9e.
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.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.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.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.
金纳米颗粒(GNPs)被广泛应用于生物学研究和应用中。由于生物安全问题,GNPs在体内的浓度通常较低,这给成像带来了挑战。这项工作研究了基于光子计数探测器(PCD)的CT(PCCT)中用于低浓度GNPs定量的最佳能量阈值选择。我们推导了金图像中物质分解误差上限的数学表达式。对具有不同GNP浓度插入物的圆柱形体模进行了全面模拟。在实际的临床前CT剂量范围内,用140 kVp的X射线束对该体模进行CT扫描。针对2通道和3通道PCCT列举了30至110 keV的PCD能量阈值,并通过寻找最低分解误差来确定最佳能量阈值。对于2通道PCCT,使金图像分解误差最小化的最佳能量阈值为44 keV,对于3通道情况为{34,40}keV。数值结果也验证了推导的分解误差上限。这项工作满足了在临床前PCCT中选择合适能量阈值以准确量化造影剂分布的需求。物质分解误差上限的解析表达式和模拟结果均表明,在选择合适的能量阈值以实现最准确的物质分解时,需要平衡考虑光子计数噪声水平和分解矩阵的数值特性。