| Literature DB >> 28740907 |
Ilana Feain1, Chun-Chien Shieh1, Paul White2, Ricky O'Brien1, Sandra Fisher2, William Counter1, Peter Lazarakis1, David Stewart2, Simon Downes2, Michael Jackson3, Siddhartha Baxi4, Brendan Whelan1,5, Kuldeep Makhija1, Chen-Yu Huang1, Michael Barton5, Paul Keall1.
Abstract
PURPOSE: The purpose of this article is to present the first imaging experiments to demonstrate the functional equivalence between a conventional rotational gantry and a fixed-beam imaging geometry, and the feasibility of an iterative image-reconstruction technique under gravitational deformation. METHODS AND MATERIALS: Experiments were performed using an Elekta Axesse with Agility MLC and XVI, a custom-built rotating phantom stage, a Catphan QA phantom, and a porcine heart. For the imaging equivalence, a conventional cone beam computed tomography (CBCT) of the Catphan was acquired, as well as a set of 660 x-ray projections with a static gantry and rotating Catphan. Both datasets were reconstructed with the Feldkamp-Davis-Kress (FDK) algorithm, and the resultant volumetric images were compared using standard metrics. For imaging under gravitational deformation, a conventional CBCT of the Catphan and a set of 660 x-ray projections with a static gantry and rotating Catphan were also acquired with a porcine heart. The conventional CBCT was reconstructed using FDK. The projections that were acquired with the heart rotating were sorted into angular bins and reconstructed with prior image constrained compressed sensing using a deformation-blurred FDK prior. Deformation was quantified with B-spline transformation-based deformable image registration.Entities:
Year: 2016 PMID: 28740907 PMCID: PMC5514241 DOI: 10.1016/j.adro.2016.10.004
Source DB: PubMed Journal: Adv Radiat Oncol ISSN: 2452-1094
Figure 1Comparison between our static gantry linac solution (left) and a conventional linac (right).
Figure 2Our small arc imaging solution in which projections are sorted into angular bins and reconstructed into separate digital-tomosynthesis images.
Figure 3(A) Reconstructed Catphan images acquired with the conventional CBCT acquisition (left) and the static gantry acquisition (middle) (C/W = −250/1500 HU). The difference image is shown on the right (C/W = 0/1000 HU). (B) The intensity profiles extracted along the dashed line as shown in (A). (C) The histogram of the difference image. HU: Hounsfield unit.
Figure 4Images of the porcine heart acquired with conventional cone beam computed tomography (CBCT) (top) and our static gantry acquisitions (bottom). For the conventional CBCT case, different views of one single, reconstructed image with the porcine heart fixed at 0 degrees is shown. For the static gantry case, a separate reconstruction from each angular bin is shown. (A) The conventional CBCT image can be considered the ground truth for the 0-degree angular bin of the static gantry, rotating phantom reconstruction. (B) For all other angular bins, gravitational deformation is expected to be the main contributing factor for the differences between the conventional CBCT image and the rotating phantom images (C/W = −250/1500 HU).