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使用¹³⁷Cs源的容积成像PET中的单光子传输

Singles transmission in volume-imaging PET with a 137Cs source.

作者信息

Karp J S, Muehllehner G, Qu H, Yan X H

机构信息

University of Pennsylvania, Department of Radiology, Philadelphia 19104, USA.

出版信息

Phys Med Biol. 1995 May;40(5):929-44. doi: 10.1088/0031-9155/40/5/014.

Abstract

The feasibility of a new method of attenuation correction in PET has been investigated, using a single-photon emitter for the transmission scan. The transmission scan is predicted to be more than a factor of ten faster with the singles method than the standard coincidence method, for comparable statistics. Thus, a transmission scan be completed in 1-2 min, rather than 10-20 min, as is common practice with the coincidence method. In addition, a potential advantage of using the single-photon source 137Cs, which has an energy of 662 keV, is that postinjection transmission studies can be performed using energy discrimination to separate the transmission from the emission data at 511 keV. In order to compensate for the energy difference of the attenuation coefficients at 662 keV compared to 511 keV, the transmission images are segmented into two compartments, tissue and lung, and known values (for 511 keV) of attenuation are inserted into these compartments. This technique also compensates for the higher amount of scatter present with the singles method, since it is not possible to use a position gate (based on collinearity of the source and two detector positions) as is commonly done with a positron-emitting source. We have demonstrated, with experimental phantom studies, that the singles transmission method combined with segmentation gives results equivalent both qualitatively and quantitatively to the coincidence method, but requires significantly less time.

摘要

已经研究了正电子发射断层扫描(PET)中一种新的衰减校正方法的可行性,该方法使用单光子发射体进行透射扫描。对于可比的统计数据,预计单光子方法的透射扫描速度比标准符合方法快十倍以上。因此,透射扫描可以在1 - 2分钟内完成,而不是像符合方法通常那样需要10 - 20分钟。此外,使用能量为662 keV的单光子源137Cs的一个潜在优势是,可以在注射后进行透射研究,利用能量鉴别从511 keV的发射数据中分离出透射数据。为了补偿662 keV与511 keV处衰减系数的能量差异,将透射图像分割为组织和肺两个部分,并将已知的(511 keV的)衰减值插入这些部分。由于无法像使用正电子发射源那样使用位置门(基于源和两个探测器位置的共线性),该技术还补偿了单光子方法中存在的较高散射量。我们通过实验模型研究表明,单光子透射方法与分割相结合,在定性和定量方面都能给出与符合方法等效的结果,但所需时间明显更少。

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