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⁹⁰Y轫致辐射单光子发射计算机断层显像成像的准直器与能量窗优化:一项SIMIND蒙特卡洛研究

Collimator and energy window optimization for ⁹⁰Y bremsstrahlung SPECT imaging: A SIMIND Monte Carlo study.

作者信息

Roshan Hoda Rezaei, Mahmoudian Babak, Gharepapagh Esmaeil, Azarm Ahmadreza, Pirayesh Islamian Jalil

机构信息

Department of Medical Physics, Faculty of Medicine, Tabriz University of Medical Sciences, Tabriz, Iran.

Department of Radiology, Radiotherapy and Nuclear Medicine, Faculty of Medicine, Tabriz University of Medical Sciences, Tabriz, Iran.

出版信息

Appl Radiat Isot. 2016 Feb;108:124-128. doi: 10.1016/j.apradiso.2015.12.041. Epub 2015 Dec 17.

Abstract

Treatment efficacy of radioembolization using Yttrium-90 ((90)Y) microspheres is assessed by the (90)Y bremsstrahlung single photon emission computed tomography (SPECT) imaging following radioembolization. The radioisotopic image has the potential of providing reliable activity map of (90)Y microspheres distribution. One of the main reasons of the poor image quality in (90)Y bremsstrahlung SPECT imaging is the continuous and broad energy spectrum of the related bremsstrahlung photons. Furthermore, collimator geometry plays an impressive role in the spatial resolution, sensitivity and image contrast. Due to the relatively poor quality of the (90)Y bremsstrahlung SPECT images, we intend to optimize the medium-energy (ME) parallel-hole collimator and energy window. The Siemens e.cam gamma camera equipped with a ME collimator and a voxelized phantom was simulated by the SImulating Medical Imaging Nuclear Detectors (SIMIND) program. We used the SIMIND Monte Carlo program to generate the (90)Y bremsstrahlung SPECT projection of the digital Jaszczak phantom. The phantom consist of the six hot spheres ranging from 9.5 to 31.8mm in diameter, which are used to evaluate the image contrast. In order to assess the effect of the energy window on the image contrast, three energy windows ranging from 60 to 160 KeV, 160 to 400 KeV, and 60 to 400 KeV were set on a (90)Y bremsstrahlung spectrum. As well, the effect of the hole diameter of a ME collimator on the image contrast and bremsstrahlung spectrum were investigated. For the fixed collimator and septa thickness values (3.28 cm and 1.14 mm, respectively), a hole diameter range (2.35-3.3mm) was chosen based on the appropriate balance between the spatial resolution and sensitivity. The optimal energy window for (90)Y bremsstrahlung SPECT imaging was extended energy window from 60 to 400 KeV. Besides, The optimal value of the hole diameter of ME collimator was obtained 3.3mm. Geometry of the ME parallel-hole collimator and energy window are indeed important indicators of the image quality in (90)Y bremsstrahlung imaging. The obtained optimal ME collimator and optimal energy window have the potential to improve the image contrast of (90)Y bremsstrahlung images. Subsequently, high quality (90)Y bremsstrahlung images can provide reliable estimate of the (90)Y microsphere activity distribution after radioembolization.

摘要

使用钇-90(90Y)微球进行放射性栓塞治疗的疗效,通过放射性栓塞后的90Y轫致辐射单光子发射计算机断层扫描(SPECT)成像来评估。放射性同位素图像有潜力提供90Y微球分布的可靠活性图。90Y轫致辐射SPECT成像中图像质量差的主要原因之一,是相关轫致辐射光子的连续且宽广的能谱。此外,准直器几何结构在空间分辨率、灵敏度和图像对比度方面起着重要作用。由于90Y轫致辐射SPECT图像质量相对较差,我们打算优化中能(ME)平行孔准直器和能量窗。配备ME准直器和体素化体模的西门子e.cam伽马相机,由模拟医学成像核探测器(SIMIND)程序进行模拟。我们使用SIMIND蒙特卡罗程序生成数字贾兹扎克体模的90Y轫致辐射SPECT投影。该体模由六个直径从9.5到31.8毫米的热球组成,用于评估图像对比度。为了评估能量窗对图像对比度的影响,在90Y轫致辐射能谱上设置了三个能量窗,范围分别为60至160千电子伏特、160至400千电子伏特和60至400千电子伏特。同样,研究了ME准直器的孔径对图像对比度和轫致辐射能谱的影响。对于固定的准直器和隔板厚度值(分别为3.28厘米和1.14毫米),基于空间分辨率和灵敏度之间的适当平衡,选择了一个孔径范围(2.35 - 3.3毫米)。90Y轫致辐射SPECT成像的最佳能量窗是6至400千电子伏特的扩展能量窗。此外,ME准直器的最佳孔径值为3.3毫米。ME平行孔准直器的几何结构和能量窗确实是90Y轫致辐射成像中图像质量的重要指标。所获得的最佳ME准直器和最佳能量窗有潜力提高90Y轫致辐射图像的对比度。随后,高质量的90Y轫致辐射图像能够提供放射性栓塞后90Y微球活性分布的可靠估计。

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