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Initial characterization of the Siemens E.CAM/sup +/: a dual-detector camera with coincidence imaging capability

机译:西门子E.CAM/sup +/-的初始特性:具有重合成像功能的双探测器摄像机

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This study characterizes the performance of the new E.CAM/sup +/ dual-gamma camera imaging system with coincidence imaging capability. This device utilizes 20.25"/spl times/14.75"/spl times/5/8" thick NaI[Tl] scintillators and slat collimators for coincidence imaging. The intrinsic spatial resolution, scatter fraction, sensitivity, count-rate capability, energy resolution and clinical image quality are evaluated. Transaxial resolution is 4.9 mm at center and does not change significantly in the radial direction and degrades to 11.4 mm tangential at source position of 20 cm for maximum detector separation of 56.8 cm. Axial resolution degrades from 4.9 mm at center to 12.2 mm at R=20 cm. Similar resolutions were measured at smaller detector separations. Scatter fraction (NEMA NU-2) was measured as 11.7%, 14.8% and 16.1% for 20%, 30% and 30%+Compton energy windows. System sensitivity, in units of cps/[/spl mu/Ci/mL] was measured as 8102, 8772 and 9740 for a 20%, 30% and 30%+Compton energy windows with a 20 cm diameter cylindrical water phantom at an activity concentration of 46 nCi/mL. Dead time losses in this phantom of 50% occur at a radioactivity concentration of 0.16 /spl mu/Ci/mL with a corresponding trues count rate of 911 cps. The true coincidence count rate peaks at 966, 1129 and 1364 cps at activity concentration of 0.24, 0.27 and 0.30 /spl mu/Ci/mL for 20%, 30% and 30%+Compton energy windows, respectively. Noise-equivalent count rate (NEC) shows a peak rate of 762, 820 and 851 cps at activity concentrations of 0.20, 0.21 and 0.19 /spl mu/Ci/mL with 20%, 30% and 30%+Compton energy windows, respectively. The system percent energy resolution degrades from 7.1% at low dead time to approximately 10% at 85% dead time. The peak center shift is less than 3% over the same dead time range. The results show that this dual-headed NaI[T1]-based gamma camera will be suitable for FDG imaging in oncologic applications with superior energy resolution but inferior sensitivity as compared to traditional cylindrical PET tomographs. Further study is required to determine optimal imaging parameters for the E.CAM/sup +/.
机译:这项研究表征了具有重合成像功能的新型E.CAM/sup + /双伽马相机成像系统的性能。该设备使用20.25“ / spl次/14.75"/spl次/ 5/8”厚的NaI [Tl]闪烁体和板条准直器进行重合成像。固有空间分辨率,散射率,灵敏度,计数率能力,能量分辨率和评估临床图像质量。轴向分辨率在中心为4.9 mm,在径向方向上没有明显变化,在20 cm的源位置处切向下降为11.4 mm,最大探测器间距为56.8 cm。轴向分辨率从在中心的4.9 mm下降在R = 20 cm时达到12.2 mm。在较小的检测器间距下测量了类似的分辨率。对于20%,30%和30%+康普顿能量窗,散射分数(NEMA NU-2)的测量值为11.7%,14.8%和16.1%系统灵敏度,以cps / [/ spl mu / Ci / mL]为单位,对于20%,30%和30%+康普顿能量窗以及直径为20厘米的圆柱水体模型,以8102、8772和9740进行测量。活性浓度为46 nCi / mL。 50%的放射性浓度为0.16 / spl mu / Ci / mL,相应的真实计数率为911 cps。分别在20%,30%和30%+ Compton能量窗口下,真实活度计数率分别在活度浓度为0.24、0.27和0.30 / spl mu / Ci / mL的966、1129和1364 cps达到峰值。当量浓度为0.20、0.21和0.19 / spl mu / Ci / mL时,等效当量计数速率(NEC)的峰值速率分别为762、820和851 cps,康普顿能量窗分别为20%,30%和30% 。系统百分比能量分辨率从低空载时间的7.1%下降到85%空载时间的大约10%。在相同的死区时间范围内,峰值中心偏移小于3%。结果表明,与传统的圆柱形PET断层扫描仪相比,这种基于NaI [T1]的双头伽马相机将适用于肿瘤学领域的FDG成像,具有较高的能量分辨率,但灵敏度较低。需要进一步研究以确定E.CAM/sup + /的最佳成像参数。

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