Developing a phenomenological model of the proton trajectory within a heterogeneous medium required for proton imaging

被引:41
作者
Fekete, Charles-Antoine Collins [1 ,2 ,3 ,4 ,5 ]
Doolan, Paul [6 ]
Dias, Marta F. [5 ,7 ]
Beaulieu, Luc [1 ,2 ,3 ,4 ]
Seco, Joao [5 ]
机构
[1] Univ Laval, Dept Phys Genie Phys & Opt, Quebec City, PQ, Canada
[2] Univ Laval, Ctr Rech Canc, Quebec City, PQ, Canada
[3] CHU Quebec, Dept Radiooncol, Quebec City, PQ, Canada
[4] CHU Quebec, CRCHU Quebec, Quebec City, PQ, Canada
[5] Massachusetts Gen Hosp, Dept Radiat Oncol, Francis H Burr Proton Therapy Ctr, Boston, MA 02114 USA
[6] UCL, Dept Med Phys & Bioengn, London, England
[7] Politecn Milan, DEIB, Milan, Italy
基金
加拿大自然科学与工程研究理事会; 加拿大创新基金会;
关键词
proton imaging; proton path estimate; proton CT; cubic spline trajectories; multiple Coulomb scattering; proton radiography; most likely path; COMPUTED-TOMOGRAPHY; MONTE-CARLO; SPATIAL-RESOLUTION; PATH; SCATTERING;
D O I
10.1088/0031-9155/60/13/5071
中图分类号
R318 [生物医学工程];
学科分类号
0831 ;
摘要
To develop an accurate phenomenological model of the cubic spline path estimate of the proton path, accounting for the initial proton energy and water equivalent thickness (WET) traversed. Monte Carlo (MC) simulations were used to calculate the path of protons crossing various WET (10-30 cm) of different material (LN300, water and CB2-50% CaCO3) for a range of initial energies (180-330 MeV). For each MC trajectory, cubic spline trajectories (CST) were constructed based on the entrance and exit information of the protons and compared with the MC using the root mean square (RMS) metric. The CST path is dependent on the direction vector magnitudes (\P-0,P-1\). First, \P-0,P-1\ is set to the proton path length (with factor Lambda(Norm)(0,1) = 1.0). Then, two optimal factor Lambda(0,1) are introduced in \P-0,P-1\. The factors are varied to minimize the RMS difference with MC paths for every configuration. A set of Lambda(opt)(0,1) factors, function of WET/water equivalent path length (WEPL), that minimizes the RMS are presented. MTF analysis is then performed on proton radiographs of a line-pair phantom reconstructed using the CST trajectories. Lambda(opt)(0,1) was fitted to the WET/WEPL ratio using a quadratic function (Y = A + BX2 where A = 1.01,0.99, B = 0.43,-0.46 respectively for Lambda(opt)(0), Lambda(opt)(1)). The RMS deviation calculated along the path, between the CST and the MC, increases with the WET. The increase is larger when using Lambda(Norm)(0,1) than Lambda(opt)(0,1) (difference of 5.0% with WET/WEPL = 0.66). For 230/330 MeV protons, the MTF10% was found to increase by 40/16% respectively for a thin phantom (15 cm) when using the Lambda(opt)(0,1) model compared to the Lambda(Norm)(0,1) model. Calculation times for Lambda(opt)(0,1) are scaled down compared to MLP and RMS deviation are similar within standard deviation. Based on the results of this study, using CST with the Lambda(opt)(0,1) factors reduces the RMS deviation and increases the spatial resolution when reconstructing proton trajectories.
引用
收藏
页码:5071 / 5082
页数:12
相关论文
共 15 条
[1]   GEANT4-a simulation toolkit [J].
Agostinelli, S ;
Allison, J ;
Amako, K ;
Apostolakis, J ;
Araujo, H ;
Arce, P ;
Asai, M ;
Axen, D ;
Banerjee, S ;
Barrand, G ;
Behner, F ;
Bellagamba, L ;
Boudreau, J ;
Broglia, L ;
Brunengo, A ;
Burkhardt, H ;
Chauvie, S ;
Chuma, J ;
Chytracek, R ;
Cooperman, G ;
Cosmo, G ;
Degtyarenko, P ;
Dell'Acqua, A ;
Depaola, G ;
Dietrich, D ;
Enami, R ;
Feliciello, A ;
Ferguson, C ;
Fesefeldt, H ;
Folger, G ;
Foppiano, F ;
Forti, A ;
Garelli, S ;
Giani, S ;
Giannitrapani, R ;
Gibin, D ;
Cadenas, JJG ;
González, I ;
Abril, GG ;
Greeniaus, G ;
Greiner, W ;
Grichine, V ;
Grossheim, A ;
Guatelli, S ;
Gumplinger, P ;
Hamatsu, R ;
Hashimoto, K ;
Hasui, H ;
Heikkinen, A ;
Howard, A .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT, 2003, 506 (03) :250-303
[2]  
Goudsmit S, 1940, PHYS REV, V57, P24, DOI 10.1103/PhysRev.57.24
[3]   Improved proton computed tomography by dual modality image reconstruction [J].
Hansen, David C. ;
Petersen, Jorgen Breede Baltzer ;
Bassler, Niels ;
Sorensen, Thomas Sangild .
MEDICAL PHYSICS, 2014, 41 (03)
[4]   Effects of Hounsfield number conversion on CT based proton Monte Carlo dose calculations [J].
Jiang, Hongyu ;
Seco, Joao ;
Paganetti, Harald .
MEDICAL PHYSICS, 2007, 34 (04) :1439-1449
[5]   Reconstruction for proton computed tomography by tracing proton trajectories: A Monte Carlo study [J].
Li, TF ;
Liang, ZR ;
Singanallur, JV ;
Satogata, TJ ;
Williams, DC ;
Schulte, RW .
MEDICAL PHYSICS, 2006, 33 (03) :699-706
[7]   The calibration of CT Hounsfield units for radiotherapy treatment planning [J].
Schneider, U ;
Pedroni, E ;
Lomax, A .
PHYSICS IN MEDICINE AND BIOLOGY, 1996, 41 (01) :111-124
[8]   MULTIPLE COULOMB SCATTERING AND SPATIAL-RESOLUTION IN PROTON RADIOGRAPHY [J].
SCHNEIDER, U ;
PEDRONI, E .
MEDICAL PHYSICS, 1994, 21 (11) :1657-1663
[9]   Spatial resolution of proton tomography: Methods, initial phase space and object thickness [J].
Schneider, Uwe ;
Pedroni, Eros ;
Hartmann, Matthias ;
Besserer, Juergen ;
Lomax, Tony .
ZEITSCHRIFT FUR MEDIZINISCHE PHYSIK, 2012, 22 (02) :100-108
[10]   A maximum likelihood proton path formalism for application in proton computed tomography [J].
Schulte, R. W. ;
Penfold, S. N. ;
Tafas, J. T. ;
Schubert, K. E. .
MEDICAL PHYSICS, 2008, 35 (11) :4849-4856