ArticleMedical physics2021
Rapid measurement of the low contrast detectability of CT scanners.
Article in Medical physics, 2021. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 7 papers.
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Who cites it
7 citing papers in PubMed.
- Automated measurement of detectability index in CT imaging: Development and validation.Journal of applied clinical medical physics · 2025Article
- Hybrid phantom for lung CT: Design and validation.Medical physics · 2025Article
- Model observer task-based assessment of computed tomography metal artifact reduction using a hip arthroplasty phantom.Medical physics · 2025Article
- Emergency CT Scans: Unveiling the Risks of Contrast-Associated Acute Kidney Injury.Tomography (Ann Arbor, Mich.) · 2024Article
- 3D printed phantom with 12 000 submillimeter lesions to improve efficiency in CT detectability assessment.Medical physics · 2024Article
- A dense search challenge phantom fabricated with pixel-based 3D printing for precise detectability assessment.Proceedings of SPIE--the International Society for Optical Engineering · 2023Article
- A Practical Method for Slice Spacing Measurement Using the American Association of Physicists in Medicine Computed Tomography Performance Phantom.Journal of medical physicsArticle
Corrections and comments
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Authors and funding
3 authors.
Funding
Abstract
purposeLow contrast detectability (LCD) is a metric of fundamental importance in computed tomography (CT) imaging. In spite of this, its measurement is challenging in the context of nonlinear data processing. We introduce a new framework for objectively characterizing LCD with a single scan of a special-purpose phantom and automated analysis software. The output of the analysis software is a "machine LCD" metric which is more representative of LCD than contrast-noise ratio (CNR). It is not intended to replace human observer or model observer studies.
methodsFollowing preliminary simulations, we fabricated a phantom containing hundreds of low-contrast beads. These beads are acrylic spheres (1.6 mm, net contrast ~10 HU) suspended and randomly dispersed in a background matrix of nylon pellets and isoattenuating saline. The task was to search for and localize the beads. A modified matched filter was used to automatically scan the reconstruction and select candidate bead localizations of varying confidence. These were compared to bead locations as determined from a high-dose reference scan to produce free-response ROC curves. We compared iterative reconstruction (IR) and filtered backpropagation (FBP) at multiple dose levels between 40 and 240 mAs. The scans at 60, 120, and 180 mAs were performed three times each to estimate uncertainty.
resultsExperimental scans demonstrated the feasibility of our technique. Our metric for machine LCD was the area under the exponential transform of the FROC curve (AUC). AUC increased monotonically from 0.21 at 40 mAs to 0.84 at 240 mAs. The sample standard deviation of AUC was approximately 0.02. This measurement uncertainty in AUC corresponded to a change in tube current of 4% to 8%. Surprisingly, we found that AUCs for IR were slightly worse than AUCs for FBP. While the phantom was sufficient for these experiments, it contained small air bubbles and alternative fabrication methods will be necessary for widespread utilization.
conclusionsIt is feasible to measure machine LCD using a search task on a phantom with hundreds of beads and to obtain tight error bars using only a single scan. Our method could facilitate routine quality assurance or possibly enable comparisons between different protocols and scanners.
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