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用于 160mm 宽锥形束 MDCT 剂量分布测量的伪螺旋扫描。

Pseudohelical scan for the dose profile measurements of 160-mm-wide cone-beam MDCT.

机构信息

Department of Radiology, Beth Israel Deaconess Medical Center and Harvard Medical School, 330 Brookline Ave, Boston, MA 02215, USA.

出版信息

AJR Am J Roentgenol. 2010 Apr;194(4):897-902. doi: 10.2214/AJR.09.3048.

Abstract

OBJECTIVE

Our objective was to determine what the reasonable total phantom length should be for the measurements and determination of length equilibrium, specifically for the Aquilion ONE cone-beam MDCT system.

MATERIALS AND METHODS

Radiation dose measurements of a 160-mm-wide cone-beam-MDCT scanner and its radiation dose profile require a different approach than the traditional or conventional method using thermoluminescent dosimeters or small ionization chambers, which have been suggested by some investigators. In order to obtain the radiation dose profile of a cone-beam MDCT, two key elements must be addressed: proper instrumentation for the detection of radiation beam and inclusion of the tails of the radiation dose profile. In this study, a small (2 x 2 x 0.3 mm) solid-state detector was used to measure the dose profile, which required the introduction of a stepping motor to pull the detector through the phantom. Inclusion of the tails of the radiation dose profile meant more than one standard CT dose index phantom would be required to encompass the dose profile tails as much as practically possible. In fact, at minimum, a total of five standard CT dose index (CTDI) phantoms would be required to ensure the entire dose profile is included and detected.

RESULTS

In the case of Toshiba Aquilion ONE MDCT with the maximum beam width of 160 mm, the phantom length that is required for the radiation dose profile measurement should be at least 750 mm, or 5 standard CTDI body phantoms. Current CTDI measurements utilizing 150 mm or 350 mm phantom lengths significantly underestimate the total dose of wide cone-beam MDCT.

CONCLUSION

The measurement method outlined in this study amounts to an introduction of a new CT dose profile measurement using a pseudohelical scan.

摘要

目的

本研究旨在确定对于 Aquilion ONE 锥形束 MDCT 系统的测量和长度均衡的确定,合理的总模体长度应该是多少。

材料与方法

对于 160mm 宽的锥形束 MDCT 扫描仪及其辐射剂量分布的辐射剂量测量需要采用与传统或常规方法不同的方法,一些研究人员建议使用热释光剂量计或小电离室进行测量。为了获得锥形束 MDCT 的辐射剂量分布,必须解决两个关键问题:用于检测辐射束的适当仪器以及包括辐射剂量分布的尾部。在本研究中,使用小(2×2×0.3mm)固态探测器来测量剂量分布,这需要引入步进电机将探测器穿过模体。包括辐射剂量分布的尾部意味着需要使用多个标准 CT 剂量指数(CTDI)模体尽可能多地包含剂量分布尾部。实际上,至少需要五个标准 CTDI 模体才能确保包括并检测整个剂量分布。

结果

在东芝 Aquilion ONE MDCT 的情况下,最大光束宽度为 160mm,辐射剂量分布测量所需的模体长度至少应为 750mm,或 5 个标准 CTDI 体模。目前使用 150mm 或 350mm 模体长度进行的 CTDI 测量会显著低估宽锥形束 MDCT 的总剂量。

结论

本研究中概述的测量方法相当于使用伪螺旋扫描引入了一种新的 CT 剂量分布测量方法。

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