physical aspects of imrt
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Physical Aspects of IMRT Samuel Tung, M.S. Sr. Medical Physicist - PowerPoint PPT Presentation

Physical Aspects of IMRT Samuel Tung, M.S. Sr. Medical Physicist UT MD Anderson Cancer Center 3D/IMRT Comparison IMRT Techniques Conventional Beam modifiers (wedge, partial blocks) Compensators LINAC, Proton therapy


  1. Physical Aspects of IMRT Samuel Tung, M.S. Sr. Medical Physicist UT MD Anderson Cancer Center

  2. 3D/IMRT Comparison

  3. IMRT Techniques • Conventional – Beam modifiers (wedge, partial blocks) • Compensators – LINAC, Proton therapy • Computerized MLCs – LINAC • Binary MLCs – PEACOCK, Tomotherapy • Robot-Controlled – Cyberknife • Scanning Beams – Proton therapy (IMPT)

  4. IMRT Delivery • Step and Shoot • Sliding Window • VMAT

  5. IMRT Delivery: Step and Shoot

  6. IMRT Delivery: Sliding Window

  7. IMRT Delivery : VMAT

  8. Motivation?

  9. Benefits of Using IMRT • Dose reductions to normal tissue • Dose Escalation to target structures • Improves target coverage of complex tumor shapes, e.g. tumor wraps around brainstem or spinal cord • Ability to delivers different doses to different targets • Ideal for reducing doses to critical structures

  10. IMRT Inverse Planning • Optimization Process for Fixed Field IMRT • Beamlet Based Optimization • Direct Aperture Optimization (DAO)

  11. The Beamlet Model • Before an IMRT optimization, each beam is defined and divided into a number of smaller beamlets (pencil beams), usually 5 mm x 5 mm

  12. The Beamlet Model • The corresponding dose distributions from all beamlets are computed and added together.

  13. The Beamlet Model • Beamlet weights are optimized to produce an optimized fluence map or matrix for each beam direction.

  14. The Beamlet Two-Steps Model • Leaf Sequencing: From “ideal” fluence, the “deliverable” MLC patterns are generated map base on machine characteristics.

  15. The Beamlet Two-Steps Model • The final “full” dose is calculated from all small beam segments (control points) • Requires a large number of segments in order to simulate the “ideal” map • Small field segments cause significant degradation in the plan quality • What you see from “ideal” fluence is “NOT” what you get from small fields

  16. NOMOS CORVUS Plan (2002)

  17. NOMOS CORVUS Plan (2002)

  18. IMRT Dosimetry - Small Fields ?

  19. Dose Modeling Problem

  20. Dose Modeling Problem

  21. Dose Modeling Problem

  22. IMRT Planning Process

  23. The Beamlet Two-Steps Model • 1 st Generation IMRT was adopted by nearly all TPS in1990: • Corvus (NOMOS) – Sliding Window • Pinnacle (ADAC) – Step and Shoot • Eclipse (Varian) – Sliding Window • Plato (Nucletron) • Xio (CMS)

  24. Direct Aperture Optimization (DAO)

  25. Direct Aperture Optimization (DAO) • Inverse planning technique where both the beam shapes and the beam weights are optimized at the same time • All of the MLC delivery parameters are included in the optimization (DMPO) • Number of beam segments and minimum MU per segment can be also predefined

  26. DAO via Simulated Annealing

  27. 1 cm

  28. DMPO Constraints

  29. DMPO Summary • Plan Quality • Total cost function ↓ 50% => Better normal tissue protection with more uniform dose to all target volumes • Treatment delivery • Total MU ↓ 40% => Less Tx time • Segments ↓ 50% => Less down time

  30. VMAT / IMAT

  31. IMAT / VMAT Optimization • IMAT treatment planning represents a particular complex optimization problem. ü The size of the problem ü Dynamic motion ü Motion limitation ü The dose calculation time

  32. N and n Optimization: An Intermediate Case MU as Function of Conversion Iterations Comparison of Dose Conversion Iteration Case # 6: 5235 Parameters Case #6: 5235 Parameters N = 5 N = 8 N = 10 N = 12 N = 15 N = 5 N = 8 N = 10 N = 12 N = 15 1 1 Normalized Total O.V. 0.8 0.8 Normalized MU 0.6 0.6 0.4 0.4 0.2 0.2 0 0 0 2 4 6 8 10 12 14 16 18 20 0 5 10 15 20 Dose Conversion Iteration Dose Conversion Iteration

  33. HN cases

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