Treating moving organs with particle beams Christoph Bert GSI - - PowerPoint PPT Presentation
Treating moving organs with particle beams Christoph Bert GSI - - PowerPoint PPT Presentation
Treating moving organs with particle beams Christoph Bert GSI Helmholtz Centre for Heavy Ion Research, Department of Biophysics Darmstadt, Germany Organ motion in radiotherapy A. Constantinescu Heart beat Friday, 9:30h Scale: seconds A.
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Organ motion in radiotherapy
Gas Prostate
Gut motion
Scale: minutes
Heart beat
Scale: seconds
- A. Constantinescu
Friday, 9:30h
- A. Rucinski
Friday, 16:12h
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Organ motion in radiotherapy Respiration
Scale: seconds
2cm 4cm 6cm 8cm 10cm range
tumor beam
Respiration in particle therapy
2/28/2012 ICTR-PHE, Geneva 2012 4
Respiratory motion - beam range
range dose
photons
12C
[courtesy S.O. Grözinger, GSI]
⇒ mitigation of range / longitudinal changes essential
2/28/2012 ICTR-PHE, Geneva 2012 5
Mitigation by margins (ICRU recommendation)
GTV CTV PTV
Gross tumor volume Clinical target volume Planning target volume
ITV Internal target volume
[Rietzel et al., MGH]
Range change dependence of margins
2/28/2012 ICTR-PHE, Geneva 2012 6 [M. Koto et al. / Radiotherapy and Oncology 71 (2004)]
Original treatment plan Original TP to 5 mm shifted tumor ⇒ Margins have to incorporate range and are thus field specific
Margins incorporating range changes
- Propage CTV to ITV by manual exchange of HU-numbers
(i.e. replace lung tissue by tumor tissue) [Koto et al. 2004]
- Scattered beams:
Change of compensator + aperture to cover all motion states of 4DCT
[Engelsman et al. 2006, Mori et al. 2008]
- Beam scanning, single field:
ITV = union of CTVs in water-equivalent space
[Bert & Rietzel 2007]
- Beam scanning, IMPT:
Beam specific WEPL-LUT and common geometric ITV [Graeff et al., GSI]
2/28/2012 ICTR-PHE, Geneva 2012 7
additional motion mitigation needed
ICTR-PHE, Geneva 2012 Geometry Water-Equivalent Path Length A B C (ref) Union of A,B,C Geometric union in WEPL of C Motion Phase
Water-equiv. Path Length ITV
[Graeff et al., GSI] 2/28/2012 8
WEPL-LUT Field 1 Field 2
CTV bone ITV
Field specific WEPL-LUT
2/28/2012 ICTR-PHE, Geneva 2012 9 [Graeff et al., GSI]
Static Dose: DVH
End Exhale (Reference) End Inhale
2/28/2012 10 ICTR-PHE, Geneva 2012 [Graeff et al., GSI]
Static Dose: ITV Comparison
Range-ITV Geo-ITV End-Inhale
11 2/28/2012 ICTR-PHE, Geneva 2012 [Graeff et al., GSI]
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4D-Dose (15 rescans): ITV Comparison
Range-ITV Geo-ITV
2/28/2012 ICTR-PHE, Geneva 2012 [Graeff et al., GSI]
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4D-Dose (15 rescans): DVH
2/28/2012 ICTR-PHE, Geneva 2012 [Graeff et al., GSI]
2/28/2012 ICTR-PHE, Geneva 2012 14
Interplay - simulation data
→ IM / ITV / PTV not sufficient
[Bert et al, Phys Med Biol, 2008]
Motion mitigation techniques
- Rescanning [Phillips et al., Phys Med Biol 1992]
- multiple scans of ITV
- several modalities investigated recently
[Seco et al. 2009, Furukawa et al. 2010, Zenklusen et al. 2010]
- Beam Tracking [Grözinger et al., Phys. Med. Biol. 2006]
- compensate target motion by real-time adjustment of Bragg peak
- 4D treatment plan optimization required
- Gating [Minohara et al., IJROBP 2000]
- beam on, if tumor within gating window
(e.g. 30% around end-exhale)
- used at NIRS for scattered beams >10 years
- reduced ITV size
- beam scanning: mitigation of residual motion
2/28/2012 ICTR-PHE, Geneva 2012 15
Motion mitigation techniques
- Abdominal compression
- supress motion
- used at HIT for treatment of
hepato cellular cancer
- scanned beam: influence of
residual motion
- Apnea
- anesthetized and intubated patient
- used at RPTC, Munich since > 1 year
- Breath hold
- could be an option for sites with fast delivery (e.g. PSI with 80ms
energy change time or NIRS with energy change on flat-top)
2/28/2012 ICTR-PHE, Geneva 2012 16
Rescanning
2/28/2012 ICTR-PHE, Geneva 2012 17 [courtesy of A. Knopf, PSI and Knopf et al. Phys Med Biol 2011]
2/28/2012 ICTR-PHE, Geneva 2012 18 [courtesy of A. Knopf, PSI and Knopf et al. Phys Med Biol 2011]
2/28/2012 ICTR-PHE, Geneva 2012 19 [courtesy of A. Knopf, PSI]
Beam Tracking
- Incorporated into GSI TPS TRiP4D
- Implemented and experimentally validated at GSI for C12
irradiations of simple geometries
- Procedure: pre-calculate compensation data for each
combination of beam position and 4DCT motion state
2/28/2012 ICTR-PHE, Geneva 2012 20
[Bert & Rietzel, Radiat Oncol 2007; Saito et al.. Phys Med Biol 2009; Bert et al. Med Phys 2007]
2/28/2012 ICTR-PHE, Geneva 2012 21
Real-time dose compensated beam tracking (RDBT)
- Real-time dose compensation necessary (RDBT)
– Beam tracking: change of beam position and energy – RDBT: additionally change of deposited dose i.e. change of all treatment plan parameters based on target motion state and pre-calculated data
- Dose change depends on temporal correlation between beam
and tumor motion
[Lüchtenborg et al. Med. Phys. 2011]
Beam tracking technique comparison
- Treatment planning study (TRiP4D)
based on 4DCT data of 5 patients
(courtesy MDACC, L.Dong)
- Modalities
- Beam Tracking (BT)
- RDBT (dose compensated BT)
- lateral BT (no range compensation)
- interplay
- Plan design:
- 4 fields, 4 fractions
- 8.2 Gy (RBE) / fraction
- based on NIRS protocol
- 81 motion combinations calculated
- Report of V95
2/28/2012 ICTR-PHE, Geneva 2012 22
[Lüchtenborg PhD-Thesis 2011]
Stationary dose distribution
Patient #5
V95
interplay RDBT
2/28/2012 ICTR-PHE, Geneva 2012 23
4D dose calculation: beam tracking
[Lüchtenborg et al., PhD-Thesis, 2011]
Results V95
- BT and RDBT
yield CTV coverage (with RBE-weighted dose)
- RDBT not
essential for lung cancer treatment
- lat. BT
sufficient for some patients
2/28/2012 ICTR-PHE, Geneva 2012 24
[Lüchtenborg PhD-Thesis 2011]
2/28/2012 ICTR-PHE, Geneva 2012 25
Gating: clinical for passively shaped beams
[Minohara et al., IJROBP 2000, Miyamoto et al., Radioth. Oncol. 2003, IJROBP 2007, Mori et al. IJROBP 2008 ]
- NIRS (Chiba, Japan) uses gating for respiration influenced
tumors since >10 years
- Passively shaped carbon beams
– No interference with target motion / simultaneous irradiation – Margins/PTV to account for motion amplitude – Compensator smearing to account for range changes
- Great clinical results
for lung cancer
– Dose escalation studies – Hypo-fractionation studies
2/28/2012 ICTR-PHE, Geneva 2012 26
Gating: Residual motion – scanned beams Irradiation under abdominal compression, e.g. liver cancer (HCC) similar residual motion
time residual motion (gating) residual motion (abd. compr.)
<~10mm
mitigation & robustness studies needed!
amplitude
2/28/2012 ICTR-PHE, Geneva 2012 27
Residual Motion Mitigation Optimize beam overlap:
F (FWHM) = 5 x ΔS beam spots ΔS ΔS F = 3 x ΔS
(standard)
(ΔS = grid spacing)
[Bert et al., IJROBP 2010]
2/28/2012 ICTR-PHE, Geneva 2012 28
Residual Motion Mitigation
beam ripple filter increased longitudinal overlap modulated bragg peak width energy layers
larger peak width B
width B
reduced slice spacing ∆Z [courtesy D. Richter, GSI]
spacing ∆Z
2/28/2012 ICTR-PHE, Geneva 2012 29
Gating-Experiments at HIT
Measured:
- ellipsoidal target volume
- 3D target motion
- 18 beam overlap
parameter combinations
- motion amplitutes up to
10 mm ⇒ ∼ 90 different parameter combinations Simulated (TRiP4D):
- additional motion
amplitudes
- 4 – 30 starting phases
⇒ ~ 900 different parameter combinations
Robot Beam Geiger Counter Target Volume 24 Ionisation Chambers Laser Sensor Anzai- Laser Sensor
2/28/2012 ICTR-PHE, Geneva 2012 30
Influence of residual motion
[Steidl, Richter, Gemmel, Bert, GSI/Siemens]
CTV PTV
2/28/2012 ICTR-PHE, Geneva 2012
Validation: Measured vs. TRiP4D calculated
Amplitude: 10mm (peak-peak) mean deviation: 0.0 ± 3.3% Amplitude: 4mm (peak-peak)
mean deviation: 2.5 ± 2.2 % beam 24 ionization chambers
Absolute Deviation
[Richter et al, Radioth. Oncol. 96(S1) 2010]
⇒ validated simulations
31
2/28/2012 ICTR-PHE, Geneva 2012 32
Example: Variation of beam focus
F=5 mm F=8 mm F=10 mm variation of ϕ0
[Steidl, Richter, Gemmel, Bert, GSI/Siemens]
residual motion [mm] homogeneity
2/28/2012 ICTR-PHE, Geneva 2012 33
Beam parameters – results
Variation grid spacing Variation beam focus Variation Bragg-Peak-width Variation IES spacing Order of influence: beam focus F > IES spacing ΔZ > grid spacing ΔS > Bragg-Peak width B
[Steidl, Richter, Gemmel, Bert, GSI/Siemens]
slope of linear fit [mm-1 ]
Hepato Cellular Cancer treatment at HIT
- HCC treatments started ~ 6 month ago, 6 patients so far
- Protocol based on NIRS experience
- 4 fractions each 8.1 Gy (RBE) (LEM I)
- Beam delivery
- abdominal press (5 pat.)
- Gating (1 pat.)
- Motion surrogate:
ANZAI belt
- Treatment QA
- 4DPET
- Ch. Kurz, Friday 12:00h
- reconstruction of daily
4D dose distribution
2/28/2012 ICTR-PHE, Geneva 2012 34
ANZAI belt
Example – abdominal compression
Δs=2mm, Δz=3mm, F=10mm Δs=2mm, Δz=3mm, F=6mm
[Richter, Härtig, Chaudhri, et al., GSI/HIT/RadioOnkol] 2/28/2012 ICTR-PHE, Geneva 2012 35
Example – Gating – 3D dose
PTV CTV
2/28/2012 ICTR-PHE, Geneva 2012 36 [Richter, Härtig, Chaudhri, et al., GSI/HIT/RadioOnkol]
Gating: 30%Ex->70In% GW (ANZAI based)
2/28/2012 ICTR-PHE, Geneva 2012 37 [Richter, Härtig, Chaudhri, et al., GSI/HIT/RadioOnkol]
2/28/2012 ICTR-PHE, Geneva 2012 38
Summary
- Particle therapy: Organ motion requires dedicated solutions
- Range influence
- Scanned beam: interplay ⇒ under-dosage
- Motion mitigation techniques
– Rescanning, gating and beam tracking + combinations – Apnea (used at RPTC for respiratory motion), abdominal compression (used at HIT for HCC) – Gating patient treatments with scanned beams started at HIT in 2011
- Still an active field of research
– Sensitivity of techniques against uncertainties – Reduction of dose to normal tissues – Precise motion monitoring – …
2/28/2012 ICTR-PHE, Geneva 2012 39
Acknowledgements
Medical Physics Group at GSI Biophysics
- R. Brevet, A. Constantinescu, C. Graeff, S. Hild, R. Kaderka,
- R. Lüchtenborg, D. Müssig, D. Richter, N. Saito, P. Steidl,
- J. Wölfelschneider
Colleagues at GSI
- M. Durante, G. Kraft, N. Kurz, W. Ott, U. Scheeler,
- P. Schütt, E. Schubert
Colleagues at HIT
- S. Brons, T. Haberer, P. Heeg, O. Jäkel, J. Naumann,
- R. Panse, K. Parodi