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Statistical performance evaluation and comparison of a Compton medical imaging system and a collimated Anger camera for higher energy photon imaging.

机译:统计性能评估和康普顿医学成像系统与准直安格相机的比较,用于更高能量的光子成像。

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In radionuclide treatment, tumor cells are primarily destroyed by charged particles emitted by the compound while associated higher energy photons are used to image the tumor in order to determine radiation dose and monitor shrinkage. However, the higher energy photons are difficult to image with conventional collimated Anger cameras, since a tradeoff exists between resolution and sensitivity, and the collimator septal penetration and scattering is increased due to the high energy photons. This research compares imaging performance of the conventional Anger camera to a Compton imaging system that can have improved spatial resolution and sensitivity for high energy photons because this tradeoff is decoupled, and the effect of Doppler broadening at higher gamma energies is decreased. System performance is analyzed by the modified uniform Cramer-Rao bound (M-UCRB) algorithms based on the developed system modeling. The bound shows that the effect of Doppler broadening is the limiting factor for Compton camera performance for imaging 364.4 keV photons emitted from (131)I. According to the bound, the Compton camera outperforms the collimated system for an equal number of detected events when the desired spatial resolution for a 26 cm diameter uniform disk object is better than 12 mm FWHM. For a 3D cylindrical phantom, the lower bound on variance for the collimated camera is greater than for the Compton imaginer over the resolution range from 0.5 to 2 cm FWHM. Furthermore, the detection sensitivity of the proposed Compton imaging system is about 15-20 times higher than that of the collimated Anger camera.
机译:在放射性核素治疗中,化合物首先释放出带电粒子,从而破坏肿瘤细胞,同时使用相关的高能光子对肿瘤成像,以确定辐射剂量并监测收缩。然而,由于在分辨率和灵敏度之间存在折衷,并且由于高能量光子而增加了准直器隔片的穿透和散射,因此用常规的准直安格相机难以成像更高能量的光子。这项研究将传统的Anger相机的成像性能与Compton成像系统进行了比较,该系统可以改善空间分辨率和对高能光子的灵敏度,因为这种权衡是不相关的,并且在更高的γ能量下多普勒展宽的影响减小了。基于改进的统一Cramer-Rao界限(M-UCRB)算法,基于已开发的系统模型,对系统性能进行了分析。该边界表明,多普勒展宽的影响是康普顿相机性能的限制因素,该相机对从(131)I发射的364.4 keV光子进行成像。根据界限,当一个直径为26 cm的均匀磁盘对象的所需空间分辨率优于12 mm FWHM时,对于检测到相同数量的事件,康普顿相机的性能优于准直系统。对于3D圆柱体模,在0.5至2 cm FWHM的分辨率范围内,准直相机的方差下限大于Compton想象器的方差下限。此外,所提出的康普顿成像系统的检测灵敏度比准直的安格相机的检测灵敏度高约15-20倍。

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