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A Compton camera for low energy gamma ray imaging in nuclear medicine applications.

机译:用于核医学应用中的低能伽马射线成像的康普顿相机。

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摘要

C-SPRINT is a prototype electronically-collimated imaging system that has been built using pixellated, low-noise, position-sensitive silicon as the first detector, and a sodium iodide scintillation detector ring as the second detector. The camera was intended to characterize potential performance gains of Compton cameras in nuclear medicine applications. The system consists of a single 4.5 x 1.5 x 0.03 cm3 silicon pad detector module with 2 keV energy resolution centered at the front face of a 50 cm diameter, 12 cm long NaI detector annulus. Calculations of the Uniform Cramer-Rao lower bound show that a "design Compton camera" based on our prototype can challenge existing mechanically-collimated systems at low to medium energies (∼140.5 - 400 keV) despite the deleterious effects of Doppler broadening. Measurements with our current system have yielded system sensitivity and spatial resolution estimates using 99mTc and 131I isotopes. Results showed an absolute efficiency of 1.8 x 10 -7 for 99mTc and 1.2 x 10-6 for 131I. The 99mTc value is an order of magnitude lower than predicted because of a combination of worse than expected silicon detector triggering performance, timing resolution issues, and system dead time effects. After correcting for these, efficiency predictions based on Monte Carlo analysis fall within 10% of the measured values. Spatial resolution estimates are also within 10% of analytical predictions. Measured resolution for the 99mTc point source was 15 min FWHM while in the 131I case, resolution improved to 8 mm FWHM. Extended source imaging was performed to characterize system performance under more challenging conditions. Images obtained were compared with measurements using a clinically-available mechanically collimated Anger camera. A resolution-variance study was also conducted for both isotopes. The results showed that the C-SPRINT camera performance on a per-detected photon basis was worse than the Anger camera for 99mTc but was similar for 131I, as predicted by theory. Potentially large gains in raw system sensitivity of a Compton camera similar in design to C-SPRINT could lead to substantial improvements in noise-equivalent performance of electronically-collimated cameras over mechanical systems, particularly in the energy range above 200 keV.
机译:C-SPRINT是原型的电子准直成像系统,已使用像素化的低噪声位置敏感型硅作为第一探测器,并使用碘化钠闪烁探测器环作为第二探测器构建。该摄像机旨在表征Compton摄像机在核医学应用中的潜在性能提升。该系统由一个单一的4.5 x 1.5 x 0.03 cm3硅垫检测器模块组成,能量分辨率为2 keV,位于50 cm直径,12 cm长的NaI检测器环面的正面。均匀Cramer-Rao下限的计算表明,尽管多普勒展宽有不利影响,但基于我们原型的“设计康普顿相机”仍可以挑战现有的低至中能量(〜140.5-400 keV)的机械准直系统。使用我们的当前系统进行的测量使用99mTc和131I同位素进行了系统灵敏度和空间分辨率估算。结果显示,对于99mTc,绝对效率为1.8 x 10 -7,对于131I为1.2 x 10-6。 99mTc值比预期值低一个数量级,原因是硅检测器的触发性能,预期时间问题和系统死区时间影响均比预期的要差。校正这些因素后,基于蒙特卡洛分析的效率预测将落在测量值的10%之内。空间分辨率估计值也位于分析预测值的10%以内。对于99mTc点源,测得的分辨率为15 min FWHM,而在131I情况下,分辨率提高到8 mm FWHM。进行了扩展源成像,以表征更具挑战性的条件下的系统性能。使用临床上可用的机械准直的Anger相机将获得的图像与测量结果进行比较。还对两种同位素进行了分辨率差异研究。结果表明,根据理论预测,在每次检测到的光子基础上,C-SPRINT相机的性能要比Anger相机差,但99mTc却比Anger相机差。设计类似于C-SPRINT的康普顿相机在原始系统灵敏度方面的潜在大幅度提高可能会导致电子准直相机在机械系统上的等效噪声性能的显着提高,尤其是在200 keV以上的能量范围内。

著录项

  • 作者

    LeBlanc, James Walter.;

  • 作者单位

    University of Michigan.;

  • 授予单位 University of Michigan.;
  • 学科 Engineering Nuclear.
  • 学位 Ph.D.
  • 年度 1999
  • 页码 173 p.
  • 总页数 173
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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