首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment >Comparative study using Monte Carlo methods of the radiation detection efficiency of LSO, LuAP, GSO and YAP scintillators for use in positron emission imaging (PET)
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Comparative study using Monte Carlo methods of the radiation detection efficiency of LSO, LuAP, GSO and YAP scintillators for use in positron emission imaging (PET)

机译:使用蒙特卡洛方法对正电子发射成像(PET)中使用的LSO,LuAP,GSO和YAP闪烁体的辐射探测效率进行比较研究

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The radiation detection efficiency of four scintillators employed, or designed to be employed, in positron emission imaging (PET) was evaluated as a function of the crystal thickness by applying Monte Carlo Methods. The scintillators studied were the LuSiO_5 (LSO), LuAlO_3 (LuAP), Gd_2SiO_5 (GSO) and the YAlO_3 (YAP). Crystal thicknesses ranged from 0 to 50 mm. The study was performed via a previously generated photon transport Monte Carlo code. All photon track and energy histories were recorded and the energy transferred or absorbed in the scintillator medium was calculated together with the energy redistributed and retransported as secondary characteristic fluorescence radiation. Various parameters were calculated e.g. the fraction of the incident photon energy absorbed, transmitted or redistributed as fluorescence radiation, the scatter to primary ratio, the photon and energy distribution within each scintillator block etc. As being most significant, the fraction of the incident photon energy absorbed was found to increase with increasing crystal thickness tending to form a plateau above the 30 mm thickness. For LSO, LuAP, GSO and YAP scintillators, respectively, this fraction had the value of 44.8, 36.9 and 45.7% at the 10 mm thickness and 96.4, 93.2 and 96.9% at the 50mm thickness. Within the plateau area approximately (57-59)%, (59-63)%, (52-63)% and (58-61)% of this fraction was due to scattered and reabsorbed radiation for the LSO, GSO, YAP and LuAP scintillators, respectively. In all cases, a negligible fraction (< 0.1%) of the absorbed energy was found to escape the crystal as fluorescence radiation.
机译:通过应用蒙特卡洛方法评估了正电子发射成像(PET)中采用或设计采用的四个闪烁体的辐射探测效率与晶体厚度的关系。研究的闪烁体是LuSiO_5(LSO),LuAlO_3(LuAP),Gd_2SiO_5(GSO)和YAlO_3(YAP)。晶体厚度为0至50毫米。该研究是通过先前生成的光子输运蒙特卡洛代码进行的。记录所有光子径迹和能量历史,并计算在闪烁体介质中转移或吸收的能量,以及作为二次特征荧光辐射重新分配和再转移的能量。计算各种参数,例如吸收,透射或重新分配为荧光辐射的入射光子能量的比例,每个闪烁体块内的散射与初级比率,光子和能量分布等。最重要的是,发现吸收的入射光子能量的比例增加了随着晶体厚度的增加,趋于在30mm厚度之上形成平台。对于LSO,LuAP,GSO和YAP闪烁体,该分数在10 mm厚度下分别为44.8、36.9和45.7%,在50mm厚度下分别为96.4、93.2和96.9%。在高原区域内,此部分的大约(57-59)%,(59-63)%,(52-63)%和(58-61)%是由于LSO,GSO,YAP和LSO的散射和重吸收辐射LuAP闪烁体,分别。在所有情况下,发现吸收的能量的一部分(<0.1%)可以作为荧光辐射逃逸到晶体之外。

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