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SU‐E‐J‐219: Quantitative Evaluation of Motion Effects On Accuracy of Image‐Guided Radiotherapy with Fiducial Markers Using CT Imaging
Author(s) -
Ali I,
Oyewale S,
Alsbou N,
Ahmad S,
Algan O
Publication year - 2014
Publication title -
medical physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.473
H-Index - 180
eISSN - 2473-4209
pISSN - 0094-2405
DOI - 10.1118/1.4888272
Subject(s) - imaging phantom , fiducial marker , cone beam computed tomography , physics , amplitude , nuclear medicine , medical imaging , position (finance) , optics , medicine , radiology , computed tomography , finance , economics
Purpose: To investigate quantitatively patient motion effects on the localization accuracy of image‐guided radiation with fiducial markers using axial CT (ACT), helical CT (HCT) and cone‐beam CT (CBCT) using modeling and experimental phantom studies. Methods: Markers with different lengths (2.5 mm, 5 mm, 10 mm, and 20 mm) were inserted in a mobile thorax phantom which was imaged using ACT, HCT and CBCT. The phantom moved with sinusoidal motion with amplitudes ranging 0–20 mm and a frequency of 15 cycles‐per‐minute. Three parameters that include: apparent marker lengths, center position and distance between the centers of the markers were measured in the different CT images of the mobile phantom. A motion mathematical model was derived to predict the variations in the previous three parameters and their dependence on the motion in the different imaging modalities. Results: In CBCT, the measured marker lengths increased linearly with increase in motion amplitude. For example, the apparent length of the 10 mm marker was about 20 mm when phantom moved with amplitude of 5 mm. Although the markers have elongated, the center position and the distance between markers remained at the same position for different motion amplitudes in CBCT. These parameters were not affected by motion frequency and phase in CBCT. In HCT and ACT, the measured marker length, center and distance between markers varied irregularly with motion parameters. The apparent lengths of the markers varied with inverse of the phantom velocity which depends on motion frequency and phase. Similarly the center position and distance between markers varied inversely with phantom speed. Conclusion: Motion may lead to variations in maker length, center position and distance between markers using CT imaging. These effects should be considered in patient setup using image‐guided radiation therapy based on fiducial markers matching using 2D‐radiographs or volumetric CT imaging.