利用锡滤波器降低 PET-CT 定位/特征级图像质量的 CT 辐射剂量:一项模型研究。

IF 3 2区 医学 Q2 RADIOLOGY, NUCLEAR MEDICINE & MEDICAL IMAGING
Natalie Anne Bebbington, Lone Lange Østergård, Kenneth Boye Christensen, Paw Christian Holdgaard
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引用次数: 0

摘要

背景:锡滤波器使一些独立诊断计算机断层扫描(CT)应用中的辐射剂量得以降低。然而,"低剂量 "CT 扫描通常用于正电子发射断层扫描(PET)-CT 病灶定位/特征描述(L/C),可容忍更高的噪声。因此,在这种图像质量水平下,锡滤波器允许的剂量降低可能会有所不同。研究的目的是确定在 PET-CT 中使用锡滤波器所允许的 CT 剂量降低水平,以获得与使用标准滤波器获得的临床参考标准 (CRS) L/C CT 图像质量相当的图像:使用 CRS 方案中的标准过滤对全身 CT 模型进行扫描,使用 120 kV 和 20mAs-ref 进行骨 L/C(用于 18F - 氟化钠 (NaF) PET-CT)扫描,使用 40mAs-ref 进行软组织 L/C(用于 18F - 氟脱氧葡萄糖 (FDG) PET-CT)扫描,然后使用锡滤波器在 100 kV (Sn100kV) 和 140 kV (Sn140kV) 电压下以一系列 mAs 设置进行扫描。每次扫描都要计算同等大小患者的有效剂量(ED),并通过定量(对比度-噪声比)和定性(视觉)分析确定 5 种不同组织的图像质量。计算出使用锡滤光片可实现的相对剂量减少量,以获得与 CRS 图像质量相当的图像质量:定量分析显示,在锡100千伏电压下使用锡滤波器,骨骼、肺部和软组织的剂量分别减少了50%-76%、27%-51%和8%-61%。定性分析显示,使用 Sn100kV 时的剂量减少与定量分析显示的剂量减少基本一致。总体而言,NaF 骨 PET-CT 的 CT 剂量减少了约 85%,只需 0.2mSv ED 就能进行全身 CT,而使用 Sn100kV(1.7-2.0mSv)的 FDG PET-CT CT 剂量减少了 30-40%,提供的图像质量与目前使用标准滤波的 CRS 图像相当。Sn140kV在减少CT剂量方面的价值有限:在 PET-CT 中以 L/C 级 CT 图像质量对骨、肺和软组织进行成像时,使用 Sn100kV 的锡滤波器可大幅降低 CT 剂量。除了降低晚年诱发癌症的风险外,这种剂量降低还可能影响 PET-CT 的实际应用,如横断面成像比平面成像更合理,或在年轻患者中使用 PET-CT 更合理。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
CT radiation dose reduction with tin filter for localisation/characterisation level image quality in PET-CT: a phantom study.

Background: The tin filter has allowed radiation dose reduction in some standalone diagnostic computed tomography (CT) applications. Yet, 'low-dose' CT scans are commonly used in positron emission tomography (PET)-CT for lesion localisation/characterisation (L/C), with higher noise tolerated. Thus, dose reductions permissible with the tin filter at this image quality level may differ. The aim was to determine the level of CT dose reduction permitted with the tin filter in PET-CT, for comparable image quality to the clinical reference standard (CRS) L/C CT images acquired with standard filtration.

Materials and methods: A whole-body CT phantom was scanned with standard filtration in CRS protocols, using 120 kV with 20mAs-ref for bone L/C (used in 18F-Sodium Fluoride (NaF) PET-CT) and 40mAs-ref for soft tissue L/C (used in 18F-Fluorodeoxyglucose (FDG) PET-CT), followed by tin filter scans at 100 kV (Sn100kV) and 140 kV (Sn140kV) with a range of mAs settings. For each scan, effective dose (ED) in an equivalent-sized patient was calculated, and image quality determined in 5 different tissues through quantitative (contrast-to-noise ratio) and qualitative (visual) analyses. The relative dose reductions which could be achieved with the tin filter for comparable image quality to CRS images were calculated.

Results: Quantitative analysis demonstrated dose savings of 50-76% in bone, 27-51% in lung and 8-61% in soft tissue with use of the tin filter at Sn100kV. Qualitative analysis demonstrated dose reductions using Sn100kV in general agreement with the dose reductions indicated by quantitative analysis. Overall, CT dose reductions of around 85% were indicated for NaF bone PET-CT, allowing whole-body CT at just 0.2mSv ED, and a 30-40% CT dose reduction for FDG PET-CT using Sn100kV (1.7-2.0mSv), providing comparable image quality to current CRS images with standard filtration. Sn140kV demonstrated limited value in CT dose reduction.

Conclusions: Large CT dose reductions can be made using the tin filter at Sn100kV, when imaging bone, lung and soft tissue at L/C level CT image quality in PET-CT. As well as reducing the risk of inducing a cancer in later life, such dose reductions may also impact PET-CT practice, such as justifying cross-sectional over planar imaging or justifying PET-CT in younger patients.

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来源期刊
EJNMMI Physics
EJNMMI Physics Physics and Astronomy-Radiation
CiteScore
6.70
自引率
10.00%
发文量
78
审稿时长
13 weeks
期刊介绍: EJNMMI Physics is an international platform for scientists, users and adopters of nuclear medicine with a particular interest in physics matters. As a companion journal to the European Journal of Nuclear Medicine and Molecular Imaging, this journal has a multi-disciplinary approach and welcomes original materials and studies with a focus on applied physics and mathematics as well as imaging systems engineering and prototyping in nuclear medicine. This includes physics-driven approaches or algorithms supported by physics that foster early clinical adoption of nuclear medicine imaging and therapy.
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