Needle artifact reduction during interventional CT procedures using a silver filter.

Autor: Reynoso-Mejia CA; Department of Radiology, University of Wisconsin-Madison, Madison, WI, 53705, USA., Troville J; Department of Medical Physics, University of Wisconsin-Madison, Madison, WI, 53705, USA., Wagner MG; Department of Radiology, University of Wisconsin-Madison, Madison, WI, 53705, USA.; Department of Medical Physics, University of Wisconsin-Madison, Madison, WI, 53705, USA., Hoppel B; Canon Medical Systems USA, Irvine, CA, 92618, USA., Lee FT Jr; Department of Radiology, University of Wisconsin-Madison, Madison, WI, 53705, USA.; Department of Urology, University of Wisconsin-Madison, Madison, WI, 53705, USA.; Department of Biomedical Engineering, University of Wisconsin-Madison, Madison, WI, 53705, USA., Szczykutowicz TP; Department of Radiology, University of Wisconsin-Madison, Madison, WI, 53705, USA. tszczykutowicz@uwhealth.org.; Department of Medical Physics, University of Wisconsin-Madison, Madison, WI, 53705, USA. tszczykutowicz@uwhealth.org.; Department of Biomedical Engineering, University of Wisconsin-Madison, Madison, WI, 53705, USA. tszczykutowicz@uwhealth.org.
Jazyk: angličtina
Zdroj: BMC biomedical engineering [BMC Biomed Eng] 2024 Mar 11; Vol. 6 (1), pp. 2. Date of Electronic Publication: 2024 Mar 11.
DOI: 10.1186/s42490-024-00076-y
Abstrakt: Background: MAR algorithms have not been productized in interventional imaging because they are too time-consuming. Application of a beam hardening filter can mitigate metal artifacts and doesn't increase computational burden. We evaluate the ability to reduce metal artifacts of a 0.5 mm silver (Ag) additional filter in a Multidetector Computed Tomography (MDCT) scanner during CT-guided biopsy procedures.
Methods: A biopsy needle was positioned inside the lung field of an anthropomorphic phantom (Lungman, Kyoto Kagaku, Kyoto, Japan). CT acquisitions were performed with beam energies of 100 kV, 120 kV, 135 kV, and 120 kV with the Ag filter and reconstructed using a filtered back projection algorithm. For each measurement, the CTDIvol was kept constant at 1 mGy. Quantitative profiles placed in three regions of the artifact (needle, needle tip, and trajectory artifacts) were used to obtain metrics (FWHM, FWTM, width at - 100 HU, and absolute error in HU) to evaluate the blooming artifact, artifact width, change in CT number, and artifact range. An image quality analysis was carried out through image noise measurement. A one-way analysis of variance (ANOVA) test was used to find significant differences between the conventional CT beam energies and the Ag filtered 120 kV beam.
Results: The 120 kV-Ag is shown to have the shortest range of artifacts compared to the other beam energies. For needle tip and trajectory artifacts, a significant reduction of - 53.6% (p < 0.001) and - 48.7% (p < 0.001) in the drop of the CT number was found, respectively, in comparison with the reference beam of 120 kV as well as a significant decrease of up to - 34.7% in the artifact width (width at - 100 HU, p < 0.001). Also, a significant reduction in the blooming artifact of - 14.2% (FWHM, p < 0.001) and - 53.3% (FWTM, p < 0.001) was found in the needle artifact. No significant changes (p > 0.05) in image noise between the conventional energies and the 120 kV-Ag were found.
Conclusions: A 0.5 mm Ag additional MDCT filter demonstrated consistent metal artifact reduction generated by the biopsy needle. This reduction may lead to a better depiction of the target and surrounding structures while maintaining image quality.
(© 2024. The Author(s).)
Databáze: MEDLINE
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