CLINICAL ASPECTS OF COMPACT GANTRY DESIGNS

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Transcription:

CLINICAL ASPECTS OF COMPACT GANTRY DESIGNS J. Heese, J. Wulff, A. Winnebeck, A. Huggins, M. Schillo VARIAN PARTICLE THERAPY JUERGEN HEESE

New gantry developments Viewpoint from user and vendor perspective what is important for the customer? precise dosimetry system minimum corrections simple and time efficient measurements to set up the clinical system short clinical commissioning time 2 VARIAN PARTICLE THERAPY

Clinical aspects of compact Gantry designs Agenda (focus on modulated scanning only) TPS setup for modulated scanning required measurements Spot positions Spot shapes SAD Upstream scanning Achromatic optics 3 VARIAN PARTICLE THERAPY

Modulated Scanning Commissioning of Treatment Planning System PENCIL BEAM SCANNING ALGORITHM 4 VARIAN PARTICLE THERAPY RELATIVE INTEGRATED DEPTH DOSE CALIBRATION OF DEPTH DOSE CURVES DOSE OUTPUT 2D SPOT SHAPES AT DIFFERENT DISTANCES Gaussian spots required VIRTUAL SAD; FOR SCANNING SAD-X AND SAD-Y REQUIRED IF DIFFERENT

Divergence Evolution of beam size around isocenter Linear increase of sigma with distance from nozzle Parametrized in treatment planning (linear/quadratic) 5 VARIAN PARTICLE THERAPY

Spot position accuracy Significant deviations between planned and delivered spot position will cause dose inhomogeneities Scanning correction required A. Huggins, master thesis 6 VARIAN PARTICLE THERAPY

Before Scanning Magnet Calibration 7 VARIAN PARTICLE THERAPY

After Scanning Magnet calibration 8 VARIAN PARTICLE THERAPY

Spot positions Conclusions After calibration, typically sub-mm accuracy of delivered vs planned spot positions can be achieved (at least in VARIAN systems) Not dependent on gantry angle Standard procedures exist to calibrate scanner magnets and derive corrections 9 VARIAN PARTICLE THERAPY

Spot shapes currently, all commercial treatment planning systems assume gaussian spot shapes new gantry designs might imply deviations from gaussian shapes most commercial treatment planning systems do not expect variations of the spot shape over the scan area If spots in air are non-gaussian, does multiple Coulomb scattering (MCS) help to reduce effects? 10 VARIAN PARTICLE THERAPY

Spot shapes in current scanning system Circular spots over full field size of 30cm x 40cm from 245 to 70 MeV 11 VARIAN PARTICLE THERAPY

TPS setup Spot shapes Spot shape characterization for treatment planning: one measurement per energy interval on central axis at isocenter required data can be significantly reduced: 2D gaussian fits, extraction of sigma-x, sigma-y per energy point repeated at typically 3 distances from isocenter and multiple gantry angles 12 VARIAN PARTICLE THERAPY

Spot shapes on future system Where is the limit? Dedicated TPS parametrization required: Elliptical spots (if gaussian): Could this spot shape be parametrized? need sigma-max, sigma-min and ellipse angle All parameters required over full field size Smooth variations of parameters required 13 VARIAN PARTICLE THERAPY

Multiple Coulomb Scattering Effect on spot size σ 0 surface 2mm 4mm 35cm water 8mm 9mm σ MCS : additional contribution due to multiple Coulomb scattering in water (e.g. Hong et al PMB 1996) 14 VARIAN PARTICLE THERAPY

Effects of MCS no fast reduction of sigma differences 25 25 20 20 sigma [mm] 15 10 15 10 sigma/sigma [%] 5 5 0 5 10 15 20 25 30 35 depth [cm] 15 VARIAN PARTICLE THERAPY

Spot shapes conclusion Deviations of spot shapes from gaussian need parametrization in TPS The more gaussian, the better MCS may not be sufficient to smooth out deviations (ellipticities or non gaussian shapes) In case of large deviations from gaussian shapes, a robust algorithm to determine spot centroids for scanner corrections is required 16 VARIAN PARTICLE THERAPY

SAD effects SAD in current scanning system Isocenter- Monitor distance d 17 VARIAN PARTICLE THERAPY

Clinical Aspects is a large SAD required for modulated scanning? skin dose limitations as a driver? the dose to the skin relative to the dose in the SOBP increases with decreasing effective source-to-axis distance (SAD). correct statement, but significant effect? does not consider dose enhancement in Bragg peak fluence modulation in modulated scanning multiple fields realistic tumor shapes and patient dimensions 18 VARIAN PARTICLE THERAPY

Proximal dose effects for small SAD central axis depth dose for a monoenergetic homogeneous field (Eclipse calculation with ProBeam beam model for different SADs) SAD proximal dose /a.u. peak dose / a.u. norm prox. Dose / a.u. 1 m 0.273 0.882 0.310 1.5 m 0.262 0.906 0.290 2 m 0.254 0.924 0.275 13% 19 VARIAN PARTICLE THERAPY

Effects for small SAD Phantom study with Eclipse, two opposed SFUD /IMPT fields Proximal dose enhancement of 1.5m vs 2m SAD relative to target dose for SFUD optimization: 5.7% for IMPT optimization: 1.9% 20 VARIAN PARTICLE THERAPY

What are the SAD effects in treatment planning? Phantom study with Eclipse, two opposed SFUD /IMPT fields Isodose effects Influence on lateral penumbra with collimator field patching: can be handled by treatment planning independent of SAD spherical distal edge isodoses no clinical impact 21 VARIAN PARTICLE THERAPY

short SAD Conclusion In the presented study no evidence for significant adverse effects of a short virtual SAD in modulated scanning down to 150cm has been identified 22 VARIAN PARTICLE THERAPY

Upstream scanning Variable virtual SAD Virtual SAD could be variable (dependent on scanning deflection in bending direction) Typically small impact on dosimetry due to large virtual SADs Variable SAD is typically not considered in treatment planning system Could have big impact in case of short virtual SADs Scanner magnet bending magnet isocenter 23 VARIAN PARTICLE THERAPY

Large momentum acceptance bending magnets Example: Consider a modulated scanning treatment plan which requires one layer at 180 MeV Case 1: E max 200 MeV -> bending magnet field set to 200 MeV Layer energy 180 MeV with magnet field setting of 200 MeV Case 2 E max =180 MeV-> bending magnet field set to 180 MeV layer energy 180 MeV with magnet field setting of 180 MeV Case 1 and case 2 could be two examples to produce a layer energy of 180 MeV, but there are many more as E max is variable leads to degeneracy of bending magnet current for a requested beam energy 24 VARIAN PARTICLE THERAPY

Large momentum acceptance bending magnets trajectories in bending magnet and optics for one energy could be different due to different magnetic fields Could lead to degenerated 2D correction function (e.g. scanner magnet calibration) variable virtual SAD effects in y, also effects due to different trajectories in x? Energy/range verification required (IEC 60601-2-64) 25 VARIAN PARTICLE THERAPY

Impact of additional corrections Potential mitigations CORRECTION TABLES IN TREATMENT MACHINE Additional commissioning work cost driver CORRECTION TABLES BY USER Special knowlegde and training for user required Additional responsibility for user Additional measurements for user ADDITIONAL CORRECTIONS IN TREATMENT PLANNING SYSTEM Additional work for user 26 VARIAN PARTICLE THERAPY

Summary SAD A large SAD is not a key requirement for downstream modulated scanning possible design could look like this: Small bore superconducting bend (4T) optimized downstream scanning, short SAD Upstream scanning large virtual SAD is beneficial to minimize variable SAD-y otherwise, TPS calculations or machine corrections have to be implemented Spot shape variations to be evaluated Large momentum acceptance Will have a more complicated impact. Solutions that work with minimum corrections have to be developed. 27 VARIAN PARTICLE THERAPY

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