vmat qa assessment verification - sfpmluz2016.sfpm.fr/luz/biblio/s3/05_barbeiro.pdf · 1 2 6 3...
TRANSCRIPT
A R Barbeiro1, A Ureba2, J A Baeza3, R Linares4, M Perucha4, E Jiménez-
Ortega1 and A Leal1
1. Dept. Fisiología Médica y Biofísica, University of Seville
2. Medical Radiation Physics, Stockholm University, Karolinska Institutet
3. Maastro Clinic, Maastricht, The Netherlands
4. Servicio de Radiofisica, Hospital Infanta Luisa, Seville
1st Workshop: Radiotherapy Modelling - Luz Saint Sauveur, Sep 2016
A model for assessing VMAT pre-treatment verification
systems and VMAT optimization algorithms
1
2
6
3
IntroductionVMAT and QA systems, main issues and uncertainties,
rationale for a highly accurate model.
Purpose
Material and MethodsLinac modelling, MC simulation and verification, QuAArC
phantom and QuAArC model.
Results and DiscussionQuAArC implementation with clinical cases, discretization
effect and proof of concept study.
Conclusions and future work
2 | 1st Workshop SFPM: Radiotherapy Modelling
Outline
5
Complexity of IMRT techniques is increasing.
VMAT dynamic implementation:
- Dynamic MLC motion
- Dose rate
- Gantry rotation speed
Rigorous QA correct delivery and consistency
with the planning.
demanding dose
distributions;
shorter treatment
times &
fewer MUs.
New uncertainties, associated issues
Introduction
Varying
Simultaneously
during
irradiation
Webb & McQuaid
PMB(54),2009
3 | 1st Workshop SFPM: Radiotherapy Modelling
Chandraraj et al., J Appl Clin Med Phys(12) 2011
Hammond L. et al, Clinical
Oncology(23) 2011
MatriXX, IBA
COMPASS/MatriXX,IBA
ArckChek, Sun NuclearDelta4, Scandidos
2D/3D QA systems
Boggula et al., PMB(56)
2011
4 | 1st Workshop SFPM: Radiotherapy Modelling
Introduction
Octavius, PTW
Film & Ion chamber
PTW and Scandidos websites
Dose calculation accuracy in these conditions.
Continuous delivery of a discrete calculation.Added complexity for optimization algorithms:
- more variables;
- connectivity (more or less robust solutions);
6MeV degradado
X (cm)
10 20 30 40 50 60 70 80 90
Y (
cm)
10
20
30
40
50
60
70
80
902000
4000
6000
8000
10000
12000
14000
DAO (Direct Aperture Optimization) (RapidArc ; SmartArc) FMO (Segmentation) + arc sequencing
Connectivity?
Plan degeneration!!
5 | 1st Workshop SFPM: Radiotherapy Modelling
Introduction
Explicit particle transport throughout the detailed
geometry of linac and patient models.
Scattered and transmitted radiation through the
beam modifiers – contribution of complex apertures.
6 | 1st Workshop SFPM: Radiotherapy Modelling
Monte Carlo simulation – rationale
Dose calculation accuracy:
Machine Log files
7 | 1st Workshop SFPM: Radiotherapy Modelling
Introduction
Continuous delivery of a discrete calculation:
Information recorded during irradiation: MLC leaf and/or jaws positions; gantry
angles; MU; etc.
Dose reconstruction on the patient anatomy (discretization level ≈ TPS).
(e.g. MobiusFX; MC simulation of DynaLog files for RapidArc QA with
DOSXYZnrc dynamic source, Teke et al.)
As a patient-specific QA method is controversial experimental dose
measurements.
High detection
density
High calculation
resolution
Highly accurate model based on Monte Carlo simulation of log files, andon 3D radiochromic film measurements in a specific cylindrical phantom.specific cylindrical phantom
Purpose
Log files information Full MC calculation.
Absolute and 3D relative dose measurements.
Entrance dose or fluence estimation.
QuAArC model
High spatial resolution
8 | 1st Workshop SFPM: Radiotherapy Modelling
EGSnrc/BEAMnrc: geometry modelling and 6MV beams simulation
Materials and Methods
MLC Tilt effect
Leaf lateral view
9 | 1st Workshop SFPM: Radiotherapy Modelling
EGSnrc/DOSXYZnrc: dose distributions calculation in a water phantom
10 | 1st Workshop SFPM: Radiotherapy Modelling%
Do
se
PDDs & OARs: MC vs. Measurements
Agreement ±2%
MLC models (leakadge, gap and tilt study): additional experimental measurements with radiochromic film.
11 | 1st Workshop SFPM: Radiotherapy Modelling
Materials and Methods
MC showed high
agreement with film
MC simulation
TPS LINAC MOSAIQ
BEAMnrc
BEAMDOSE
Automatic MC verification of TPS (RTP files) and log files
12 | 1st Workshop SFPM: Radiotherapy Modelling
Materials and Methods
MC simulation
TPS LINAC MOSAIQ
BEAMnrc
BEAMDOSE
Automatic MC verification of TPS (RTP files) and log files
13 | 1st Workshop SFPM: Radiotherapy Modelling
Materials and Methods
Log file
14 | 1st Workshop SFPM: Radiotherapy Modelling
Different discretization level
– effect in the verification
process.
MC simulation of Log files
15 | 1st Workshop SFPM: Radiotherapy Modelling
Different discretization level
– effect in the verification
process.
MC simulation of Log files
16 | 1st Workshop SFPM: Radiotherapy Modelling
Different discretization level
– effect in the verification
process.
MC simulation of Log files
Log file analysis
MC simulation of log files
MLC leaf positions difference between RTP and LOG
dif
feren
ce (
cm
)
Mu distribution for the entire arc
RTP MULOG MU
0
-3
-2
-1
1
2
3
4
5
6
17 | 1st Workshop SFPM: Radiotherapy Modelling
QuAArC phantom:
18 | 1st Workshop SFPM: Radiotherapy Modelling
Materials and Methods
Big setup:
30 cm x 30 cm length
Small setup:
20 cm x 28 cm length
3D relative dose
measurements & absolute
point dose measurements
Outer film scroll:entrance dose
estimation
Inner film scroll: dose distribution
19 | 1st Workshop SFPM: Radiotherapy Modelling
Materials and Methods
Dose processing and 3D dose reconstruction:
min𝑥
12𝐶 ∙ 𝑥 − 𝑑
2
2such that
𝐴 ∙ 𝑥 ≤ 𝑏𝐴𝑒𝑞 ∙ 𝑥 = 𝑏𝑒𝑞𝑙𝑏 ≤ 𝑥 ≤ 𝑢𝑏
Feedback process to experimentally
adjust MUs with measurements
20 | 1st Workshop SFPM: Radiotherapy Modelling
Materials and Methods
Feedback process – proposed MU variations for IMRT and VMAT plans.
IMRT plan VMAT plan
Clinical cases planned with different conventional TPS:
- MONACO
- PINNACLE
Verified with different commercial systems:
- Delta4
- COMPASS
Some of them were not accepted during their verification (2 treatment plansfor a same case).
21 | 1st Workshop SFPM: Radiotherapy Modelling
QuAArC model validation with clinical cases:
Materials and Methods
Final QuAArC phantom - experimental verification:
22 | 1st Workshop SFPM: Radiotherapy Modelling
Rolled up radiochromic
EBT3 films
PMMA slices for axial films
With cork cylinders
Results
23 | 1st Workshop SFPM: Radiotherapy Modelling
% Dose DifferenceFilm Dose Distributions
Ou
ter
Fil
m
0-1
80
º
γ (3%/3mm)
Ou
ter
Fil
m
18
0-3
60
º
In
ner
Fil
m0
-36
0º
Reproducibility of film scroll measuments in QuAArC.
High reproducibility:
γ < 1: > 99%
Results
24 | 1st Workshop SFPM: Radiotherapy Modelling
Discretization level effect in treatment verification:
Results – QuAArC model implementation
Gantry angle (°)
Axia
l sli
ce (
mm
)
Film vs MC Log Film vs QuAArC solution
% Dose Differences – coarse discretization
% Dose Differences – fine discretization
Film vs MC Log Film vs QuAArC solution
(a) (b) (c)
(d) (e) (f)
25 | 1st Workshop SFPM: Radiotherapy Modelling
QuAArC model implementation: coarse Vs. fine log
Results
min𝑥
12𝐶 ∙ 𝑥 − 𝑑
2
2such that
𝐴 ∙ 𝑥 ≤ 𝑏𝐴𝑒𝑞 ∙ 𝑥 = 𝑏𝑒𝑞𝑙𝑏 ≤ 𝑥 ≤ 𝑢𝑏
26 | 1st Workshop SFPM: Radiotherapy Modelling
% Dose Differences Gamma Analysis (2%/2mm)Film Dose Distributions QuAArC Dose Distributions
Gantry angle (°)
Prostate VMAT Plan
Ou
ter s
croll
In
ner s
croll
Axia
l slice
(m
m)
% Dose Differences Gamma Analysis (2%/2mm)Film Dose Distributions QuAArC Dose Distributions
Gantry angle (°)
H&N VMAT Plan
Ou
ter s
croll
In
ner s
cro
llA
xia
l slice
(m
m)
PINNACLE/COMPASS Plans
Proof of concept of the feedback process Results
Prostate
case
H&N
case
27 | 1st Workshop SFPM: Radiotherapy Modelling
DVHs PINNACLE TPS Vs. QuAArC
Results
PINNACLE/COMPASS Plans
28 | 1st Workshop SFPM: Radiotherapy Modelling
DVHs COMPASS Vs. QuAArC
Results
PINNACLE/COMPASS Plans
29 | 1st Workshop SFPM: Radiotherapy Modelling
% Dose DifferencesFilm Dose Distributions QuAArC Dose Distributions
Axia
l sli
ce
(m
m)
Gantry angle (°)
Plan A
In
ner s
croll
Plan B
Ou
ter s
croll
In
ner s
croll
Ou
ter s
croll
Gamma Analysis (2%/2mm)
Prostate caseMONACO/Delta4 Plans
ResultsProof of concept of the feedback process
min𝑥
12𝐶 ∙ 𝑥 − 𝑑
2
2such that
𝐴 ∙ 𝑥 ≤ 𝑏𝐴𝑒𝑞 ∙ 𝑥 = 𝑏𝑒𝑞𝑙𝑏 ≤ 𝑥 ≤ 𝑢𝑏
30 | 1st Workshop SFPM: Radiotherapy Modelling
% Dose Differences Gamma Analysis (2%/2mm)
Film Dose Distributions QuAArC Dose Distributions
Axia
l sli
ce
(m
m)
Gantry angle (°)
Plan A
In
ner s
croll
Plan B
Ou
ter s
croll
In
ner s
croll
Ou
ter s
croll
MONACO/Delta4 Plans
Proof of concept of the feedback process
H&N case
Results
min𝑥
12𝐶 ∙ 𝑥 − 𝑑
2
2such that
𝐴 ∙ 𝑥 ≤ 𝑏𝐴𝑒𝑞 ∙ 𝑥 = 𝑏𝑒𝑞𝑙𝑏 ≤ 𝑥 ≤ 𝑢𝑏
31 | 1st Workshop SFPM: Radiotherapy Modelling
(c) (d)
(a) (b)
ResultsDVHs for QuAArC model Vs. MONACO TPS
33 | 1st Workshop SFPM: Radiotherapy Modelling
Conclusions and future work
QuAArC model showed to be consistent and robust.
Effect of dose calculation accuracy and degree of detection density was
assessed in the developed model. (more reliable solutions, DVHs)
Potentially, control and reduce VMAT uncertainties, allowing evaluation of
commercial VMAT systems and/or the optimization algorithm implemented in
TPS.
Further studies about VMAT efficiency against more established techniques in
specific cases.
QuAArC model for dose painting verification.
QuAArC is being adapted for 4D verification.
QuAArC can also be implemented without MC.
Funding: Spanish Ministry of Science and Technology and FEDER.
Radiophysics department, Virgen Macarena Hospital, Seville.
Radiophysics department, Virgen del Rocio Hospital, Seville.
Radiophysics department, Infanta Luisa Clinic, Seville.
Thank you for your attention !
34 | 1st Workshop SFPM: Radiotherapy Modelling
Acknowledgments