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首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment >Monte Carlo investigation of positron annihilation in medical positron emission tomography
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Monte Carlo investigation of positron annihilation in medical positron emission tomography

机译:医学正电子发射断层扫描中正电子ography灭的蒙特卡洛研究

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摘要

A number of Monte Carlo codes are available for simulating positron emission tomography (PET), however, physics approximations differ. A number of radiation processes are deemed negligible, some without rigorous investigation. Some PET literature quantify approximations to be valid, without citing the data source. The radiation source is the first step in Monte Carlo simulations, for some codes this is 511 keV photons 180° apart, not polyenergetic positrons with radiation histories of their own. Without prior assumptions, we investigated electron-positron annihilation under clinical PET conditions. Just before annihilation, we tallied the positron energy and position. Right after annihilation, we tallied the energy and separation angle of photon pairs. When comparing PET textbooks with theory, PENELOPE and EGSnrc, only the latter three agreed. From 10~6 radiation histories, a positron source of ~(15)O in a chest phantom annihilated at as high as 1.58 MeV, producing photons with energies 0.30-2.20 MeV, 79-180° apart. From 10~6 radiation histories, an ~(18)F positron source in a head phantom annihilated at energies as high as 0.56 MeV, producing 0.33-1.18 MeV photons 109-180° apart. 2.5% and 0.8% annihilation events occurred inflight in the chest and the head phantoms, respectively. PET textbooks typically either do not mention any deviation from 180°, or state a deviation of 0.25° or 0.5°. Our findings are founded on the well-established Heitler cross-sections and relativistic kinematics, both adopted unanimously by PENELOPE, EGSnrc and GEANT4. Our results highlight the effects of annihilation in-flight, a process sometimes forgotten within the PET community.
机译:许多蒙特卡罗代码可用于模拟正电子发射断层扫描(PET),但是,物理近似是不同的。许多辐射过程被认为可以忽略不计,有些没有经过严格的调查。一些PET文献在没有引用数据来源的情况下将近似值量化为有效。辐射源是蒙特卡洛模拟的第一步,对于某些代码,这是相距180°的511keV光子,而不是具有自身辐射历史的多能正电子。在没有事先假设的情况下,我们研究了临床PET条件下的电子-正电子an灭。在歼灭之前,我们计算了正电子的能量和位置。 an灭后,我们计算了光子对的能量和分离角。在将PET教科书与理论,PENELOPE和EGSnrc进行比较时,只有后三者同意。从10〜6次辐射历史来看,胸部幻像中的〜(15)O正电子源​​被ni灭,最高可达到1.58 MeV,产生的光子的能量为0.30-2.20 MeV,相距79-180°。从10〜6个辐射历史来看,头部模型中的〜(18)F正电子源被an灭,能量高达0.56 MeV,从而产生109-180°的0.33-1.18 MeV光子。 2.5%和0.8%的ation灭事件分别发生在飞行中的胸部和头部幻影中。 PET教科书通常不会提到任何与180°的偏差,或陈述0.25°或0.5°的偏差。我们的发现建立在完善的海特勒横截面和相对论运动学的基础上,两者均被PENELOPE,EGSnrc和GEANT4一致采用。我们的研究结果突出了飞行中an灭的影响,这在PET社区中有时被遗忘了。

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