Moore Stephen C, Foley Kijewski Marie, El Fakhri Georges
Division of Nuclear Medicine, Department of Radiology, Brigham and Women's Hospital and Harvard Medical School, Boston, MA 02115, USA.
IEEE Trans Med Imaging. 2005 Oct;24(10):1347-56. doi: 10.1109/TMI.2005.857211.
We describe a new approach to the problem of collimator optimization in nuclear medicine; our methodology is illustrated for the challenging case of gallium-67 imaging. Collimator-design methods based on empirical rules, such as specification of an allowable level of single-septal penetration (SSP) at a fixed energy, are especially inappropriate for radionuclides characterized by an abundance of high-energy contaminant photons that scatter in the patient, collimator, and/or detector before detection within one of a few photopeak energy windows. Lead X-rays produced in the collimator are an additional source of contamination. We designed optimal collimation for 67Ga based on relevant clinical imaging tasks and a realistic simulation of photon transport in a phantom, collimator, and detector. Collimator designs were compared on the basis of performance in lesion detection, as predicted by a three-channel Hotelling observer (CHO), as well as in tumor and background activity estimation (EST), quantified by task-specific signal-to-noise ratios (SNRs). The optimal values of collimator lead content were 22.0 and 23.8 g/cm2, respectively, for CHO and EST, while the optimal geometric resolution values were 1.8 and 1.6 cm full-width at half-maximum (FWHM), respectively, at a distance of 23.5 cm. The resolution of a commercially available medium-energy low-penetration collimator (MELP) is 1.9 cm FWHM at this distance. The optimal values for SSP at 300 keV were 7.3% and 5.8% based on CHO and EST, respectively, compared to 5.2% for the MELP collimator. Compared with the commercial MELP collimator, the 67Ga collimator optimized for tumor detection or activity estimation tasks provided improved geometric spatial resolution with reduced geometric efficiency and, surprisingly, allowed an increased level of single-septal penetration.
我们描述了一种解决核医学中准直器优化问题的新方法;针对具有挑战性的镓 - 67成像案例展示了我们的方法。基于经验规则的准直器设计方法,例如在固定能量下指定允许的单隔板穿透(SSP)水平,对于以大量高能污染光子为特征的放射性核素尤其不合适,这些光子在患者、准直器和/或探测器中散射,然后在几个光电峰能量窗口之一内被检测到。准直器中产生的铅X射线是另一种污染来源。我们基于相关临床成像任务以及对体模、准直器和探测器中光子传输的真实模拟,为67Ga设计了最佳准直。根据三通道霍特林观察者(CHO)预测的病变检测性能以及通过特定任务信噪比(SNR)量化的肿瘤和背景活性估计(EST),对准直器设计进行了比较。对于CHO和EST,准直器铅含量的最佳值分别为22.0和23.8 g/cm2,而在23.5 cm距离处,最佳几何分辨率值分别为半高宽(FWHM)1.8和1.6 cm。在此距离下,市售中能低穿透准直器(MELP)的分辨率为FWHM 1.9 cm。基于CHO和EST,300 keV时SSP的最佳值分别为7.3%和5.8%,而MELP准直器为5.2%。与市售MELP准直器相比,针对肿瘤检测或活性估计任务优化的67Ga准直器在降低几何效率的情况下提高了几何空间分辨率,并且令人惊讶的是,允许更高水平的单隔板穿透。