Op#miza#on of a Fast CT System for More Accurate Radiotherapy. Erica Cherry, Meng Wu, and Rebecca Fahrig
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1 Op#miza#on of a Fast CT System for More Accurate Radiotherapy Erica Cherry, Meng Wu, and Rebecca Fahrig
2 Problem: mo#on during treatment Two overlapping thorax views during normal breathing liver lung spine lung K.K. Brock, Imaging and Image- Guided Radia7on Therapy in Liver Cancer, 2011
3 Fix: PHASER PHASER = Pluridirec#onal High- Energy Agile Scanning Electron Radiotherapy Basic idea: deliver en#re radia#on treatment in a few seconds to effec#vely freeze mo#on Mechanism: use high- energy electrons, which can be steered electronically (no moving parts) 100 MeV electrons can deliver a dose with similar accuracy to 2 MeV photons (mean energy)
4 PHASER Setup Array of high energy electron source lines Region of interest Diverging electron beam Not shown: pa#ent table, beam stop, imaging system, outer casing
5 Work Flow Acquire pre- treatment raw data Adjust therapy plan Reconstruct image Deliver therapy Register image Verify correct #ssue was irradiated
6 Goals of Pre- Treatment Imaging System Acquire a high- quality image to adjust treatment plan Image within a breath hold Adequate contrast to iden#fy important structures 40- cm axial FOV, 50- cm diameter pa#ent Acquire a fast- image of the the tumor to verify posi#on immediately prior to treatment Speed is more important than quality 10- cm axial FOV, 50- cm diameter pa#ent Don t break the bank: 64- slice scanner ~ $1 million, 128- slice scanner ~ $2 million* * The internet, don t quote this
7 Geometry 1: Helical Scan pitch = cm x x x y Detector arclength =102.3 cm z 6.4 cm y z Axial field of view = 40 cm In- plane field of view = 50 cm (diameter)
8 Geometry 2: Cone Beam Scan No axial mo#on cm x x x y z 12.8 cm Axial field of view = 10 cm In- plane field of view = 50 cm (diameter) y z
9 Parameter Summary Parameter Clinical Scanner PHASER Scanner Source to detector distance Detector rows/ pixel size 1040 mm (too small to laterally shif pa#ents) 64 rows, 1 x 1 mm 2 (FOV too small) Pixels/row ($$$) 512 Voxel size mm 3 at detector (unnecessary resolu#on, $$$) 1300 mm 16 low res (4 x 4 mm 2 ) + 32 higher res (2 x 2 mm 2 ) + 16 low res (4 x 4 mm 2 ) 2.0 mm 3 at detector An#scaker grid Varies 2D, 35 mm lamellae
10 CT Simula#on with XCAT Phantom Full dataset is the sum of two simula#ons Primary photons (determinis#c) Scakered photons (Monte Carlo) Numerical phantom used to simulate pa#ent
11 Primary Simula#on Sofware generates cone beam projec#on images, includes tools for 3D volume reconstruc#on, DOES NOT include scaker X- ray akenua#on, one energy, one material I(L) = I 0 exp( µl) X- ray akenua#on, polyenerge#c, several materials E max I(x tot ) = I 0,E E min n exp( µie L i )de i=1 Polychroma#c X- ray source Akenua#on caused by passage through material Detector captures akenuated rays
12 Scaker Simula#on: Why Bother? Ideal CT: X- rays either go straight to detector or are absorbed Real CT: Some x- rays are deflected to the wrong detector loca#on Source Detector Source Detector
13 More About Scaker Most accurately modeled with a Monte Carlo simula#on (accounts for random physical processes responsible for scakering) Can be reduced with an an#- scaker grid (see right) Source Curved detector with an#- scaker grid
14 Results Phantom Primary only Primary and scaker Scaker corrected
15 Results: Shoulders Primary only Primary and scaker Scaker corrected Current system
16 Results: Lungs, middle Primary only Primary and scaker Scaker corrected Current system
17 Results: Lungs, bokom Primary only Primary and scaker Scaker corrected Current system
18 Conclusions Current system design produces reasonable image quality fast and at a reasonable price Some remaining work on cone beam and trunca#on ar#fact reduc#on Extremely general CT simula#on can evaluate image quality in other new systems
19 Future Work Simulate imaging phantoms with low- contrast tumors and use system to evaluate ease of lesion recogni#on Apply system to real pa#ent data Next step of imaging pipeline: use registra#on sofware to compare registra#on accuracy with XCAT phantoms and real pa#ent data
20 Acknowledgements Meng Wu and Rebecca Fahrig PHASER team Stanford Cancer Imaging Training Fellowship Department of Defense
21 Ques#ons?
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