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狭缝平板准直器关于调制传递函数的优化。

Slit slat collimator optimization with respect to MTF.

作者信息

Kamali-Asl A, Sarkar S, Shahriari M, Agha-Hosseini H

机构信息

Physics Department, Amir-Kabir University, Tehran, Iran.

出版信息

Appl Radiat Isot. 2005 Mar;62(3):461-8. doi: 10.1016/j.apradiso.2004.07.009.

Abstract

Conventional single photon emission computed tomography (SPECT) collimators are not suitable for 511 keV imaging. In order to use a SPECT system for single positron emission tomography (SPET), we need to design high-efficiency collimators capable of absorbing 511 keV photons. Slit slat (SS) collimators have been proposed for this purpose even though the optimization of such collimators has not yet been performed. In order to investigate the reliability of the system with SS collimator, it was decided to evaluate such a system. A gamma camera system with both parallel hole (PH) and SS collimators was simulated by Monte Carlo method. In these simulation parameters of the simulated system having 3/8 in NaI(Tl) crystal for 140 keV gamma-rays with PH collimator was compared with practical results and a good correlation was found between the simulated and practical results. In this way, the validity of our simulation code was confirmed. The crystal thickness for simulated gamma-camera system with SS collimator for detection of 511 keV photons was set to be 5/8 in which resulted in an intrinsic spatial resolution of 4mm. The simulated SS collimators consisted of 50 lead plates of various height, thickness and spacing. The imaging was performed by rotating the SS collimator from 0 degrees to 180 degrees in 73 steps of 2.5 degrees each. The physical parameters such as spatial resolution, efficiency and modulation transfer function (MTF) of this system for different SS collimator designs, (i.e. SS(64,3,3), SS(80,3,3), SS(64,4,5), SS(80,4,5), SS(85,4,5), where in SS(h,s,t) is used to indicate the septal height (h), septal separation (s), and septal thickness (t) in millimeters were evaluated. The value of these parameters were compared with the values obtained employing a 511 keV PH(85,4,2.5) collimator. Based on MTF values, our result showed that the SS(85,4,5) collimator has an optimum performance to the other SS collimators. The relative efficiency of the system with SS(85,4,5) collimator was about 20 times higher than the efficiency of the system with the PH(85,4,2.5) collimator whereas in this case the spatial resolution had deteriorated by almost 8% (i.e. from 14.1 to 15.0 mm). The result of this study shows that the SS collimators have great advantages over the conventional PH collimators for 511 keV imaging, providing much higher efficiency while maintaining a comparable spatial resolution. Employing this collimator makes it possible to use a SPECT system for metabolic imaging by SPET system.

摘要

传统的单光子发射计算机断层扫描(SPECT)准直器不适用于511keV成像。为了将SPECT系统用于单光子发射断层扫描(SPET),我们需要设计能够吸收511keV光子的高效准直器。为此已提出了狭缝平板(SS)准直器,尽管此类准直器尚未进行优化。为了研究带有SS准直器的系统的可靠性,决定对这样一个系统进行评估。通过蒙特卡罗方法模拟了一个同时具有平行孔(PH)准直器和SS准直器的伽马相机系统。在这些模拟中,将具有3/8英寸碘化钠(铊)晶体用于140keV伽马射线且带有PH准直器的模拟系统的参数与实际结果进行了比较,发现模拟结果与实际结果之间具有良好的相关性。通过这种方式,证实了我们模拟代码的有效性。用于检测511keV光子的带有SS准直器的模拟伽马相机系统的晶体厚度设置为5/8英寸,其固有空间分辨率为4mm。模拟的SS准直器由50块具有不同高度、厚度和间距的铅板组成。通过将SS准直器以2.5度的步长从0度旋转到180度来进行成像。对该系统针对不同SS准直器设计(即SS(64,3,3)、SS(80,3,3)、SS(64,4,5)、SS(80,4,5)、SS(85,4,5),其中在SS(h,s,t)中用于表示间隔高度(h)、间隔间距(s)和间隔厚度(t),单位为毫米)的物理参数,如空间分辨率、效率和调制传递函数(MTF)进行了评估。将这些参数的值与采用511keV PH(85,4,2.5)准直器获得的值进行了比较。基于MTF值,我们的结果表明,SS(85,4,5)准直器相对于其他SS准直器具有最佳性能。带有SS(85,4,5)准直器的系统的相对效率比带有PH(85,4,2.5)准直器的系统的效率高约20倍,而在这种情况下空间分辨率下降了近8%(即从14.1mm降至15.0mm)。这项研究的结果表明,对于511keV成像,SS准直器相对于传统的PH准直器具有很大优势,在保持相当空间分辨率的同时提供了更高的效率。采用这种准直器使得能够将SPECT系统用于SPET系统的代谢成像。

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