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Published byShannon Newman Modified over 9 years ago
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Pencil-Beam Redefinition Algorithm Robert Boyd, Ph.D.
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Pencil Beam Algorithms
central axis of broad beam (Z) X pixel bounding pencil beams (2x2 mm2 at isocenter) Y Z X-Y plane normal to beam axis (Z)
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Pencil Beam Redefinition
DX Z Z+DZ X-Y planes are spaced 5 mm apart on Z axis
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PBRA Physics Primary electron transport only
delta-rays not modeled Multiple Coulomb scattering approximated with a Gaussian distribution large-angle scattering not modeled Mean collisional energy loss only catastrophic energy losses not modeled
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PBRA Physics Approximations
PBRA requires measured central-axis depth dose curve PBRA uses an energy-dependent correction factor C(E) to match calculated and measured central axis depth dose curve
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Polyenergetic Spectrum
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PBRA Correction Factor C(E)
Solid Line: Monoenergetic PBRA C(E) Dashed Line: Polyenergetic PBRA C(E)
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Polyenergetic PBRA
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20-MeV Horizontal Bone Slab
Varian Clinac 2100, 15x15-cm2 open applicator, 100 cm SSD
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20-MeV Horizontal Bone Slab
Varian Clinac 2100, 15x15-cm2 open applicator, 100 cm SSD
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20-MeV Horizontal Air Slab
Varian Clinac 2100, 15x15-cm2 open applicator, 100 cm SSD
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20-MeV Vertical Air Slab Varian Clinac 2100, 15x15-cm2 open applicator, 100 cm SSD
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20-MeV Vertical Air Slab Off-axis profile at 4.5 cm depth
Varian Clinac 2100, 15x15-cm2 open applicator, 102 cm SSD
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20-MeV Nose Surface Varian Clinac 2100, 15x15-cm2 open applicator, 100 cm SSD
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9-MeV Nose Surface Off-axis profile at 1 cm depth
Varian Clinac 2100, 15x15-cm2 open applicator, 100 cm SSD
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PBRA Evaluation with Measured Data Set - Results
PBRA was not able to achieve 4% or 2 mm dose calculation accuracy for all data points
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Beam Modeling electron source SADvir custom beam collimation L0
isocenter patient
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Dual-Source Beam Modeling
primary electron source secondary electron source custom beam collimation isocenter patient
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Dual-Source Model - 100 cm SSD
Varian Clinac 1800, 9 MeV, 6x6-cm2 open applicator
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Dual-Source Model - 110 cm SSD
Varian Clinac 1800, 9 MeV, 6x6-cm2 open applicator
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IMC - Transverse Plane Varian 2100, 16 MeV, 15x15-cm2 applicator, 105 cm SSD
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IMC - Transverse Plane Varian 2100, 16 MeV, 15x15-cm2 applicator, 105 cm SSD
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IMC - Sagittal Plane Varian 2100, 16 MeV, 15x15-cm2 applicator, 105 cm SSD
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IMC - Sagittal Plane Varian 2100, 16 MeV, 15x15-cm2 applicator, 105 cm SSD
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Parotid Gland - Transverse View
Varian 2100, 16 MeV, 15x15-cm2 applicator, 100 cm SSD
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Parotid Gland - Transverse View
Varian 2100, 16 MeV, 15x15-cm2 applicator, 100 cm SSD
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Ethmoid Sinuses - Transverse Plane
Varian 2100, 16 MeV, 10x10-cm2 applicator, 100 cm SSD
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Ethmoid Sinus - Transverse Plane
Varian 2100, 16 MeV, 10x10-cm2 applicator, 100 cm SSD
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Ethmoid Sinus - Profile at Y = 13.0 cm
Varian 2100, 16 MeV, 10x10-cm2 applicator, 100 cm SSD
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Clinical Evaluation - Results
Accuracy criteria was not achieved for entire irradiated volume, albeit only a small volume (< 3.5%) had dose differences greater than 4% and greater than 2 mm DTA. PBRA showed good agreement with Monte Carlo in matching isodose lines. Better modeling of physics will improve the accuracy of PBRA-calculated dose.
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Custom Bolus / Skin Collimation
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Custom Bolus / Skin Collimation
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Custom Bolus / Skin Collimation
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Custom Bolus / Skin Collimation
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Electron Arc Therapy
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Skin Collimation
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Arc Therapy with Skin Collimation
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Pencil-Beam Divergence Current PBRA
virtual source distance is equal to distance to broad beam virtual source mathematics assume “parallel”point beams integration performed over projected area svir Dx Dz
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Pencil-Beam Divergence divPBRA
virtual source distance is a pencil beam-specific parameter mathematics assume divergent point beams integration performed over normal pixel width svir Dx Dz
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Local Pencil-Beam Divergence
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20-MeV Horizontal Air Slab
Varian Clinac 2100, 15x15-cm2 open applicator, 100 cm SSD
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Pencil-Beam Divergence Results
divPBRA was more accurate than PBRA for most data points divPBRA was not able to achieve 4% or 2 mm accuracy for all data points Calculation times were approximately 30% longer
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Arc Beam Modeling
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Future Work Dosimetry studies using PBRA
Tomotherapy vs. conventional electron therapy Field matching for chest wall treatments Electron arc therapy planning using divPBRA Realistic dose deposition kernels using Monte Carlo Automated custom bolus/skin collimation planning using PBRA Translating PBRA to commercial system
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Acknowledgements Kenneth Hogstrom, Ph.D. Almon Shiu, Ph.D.
Dennis Leavitt, Ph.D. Mitch Price, M.S. Melinda Chi, M.S Paul Alderson, B.S.
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