Discuss the general planning concepts used in proton planning. Review the unique handling of CTV / ITV / PTV when treating with protons

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Transcription:

Mark Pankuch, PhD

Discuss the general planning concepts used in proton planning Review the unique handling of CTV / ITV / PTV when treating with protons Pencil Beam distributions and PBS optimization

Cover the target with appropriate margins Spare the critical structures Plan with fields that deliver the most robust plan

Protons Range : The depth of the Bragg peak (D90%) Modulation : The spread of the Bragg peak Compensators : Distal Shaping Patch Fields : Distal Edge to Lateral Edge Matching IMPT : Inverse planning method

Relative Dose Spread Out Bragg Peak (SOBP) 100 80 60 40 20 0 Healthy Tissue Tumor 0 5 10 15 20 25 30 Depth in Tissue (cm) Healthy Tissue

7

Patient Specific Devices Aperture

1 0.8 0.6 0.4 0.2 2 cm 20 cm 40 cm 0-8 -6-4 -2 0 2 4 6 8 Distance (cm)

Relative Intensity Penumbra at Various Ranges, mid-sopb (4cm) 1 0.9 0.8 0.7 0.6 0.5 0.4 Range 10cm Range 20cm Range 30m 0.3 0.2 0.1 0 Distance (cm)

Target Area Proton Beam Aperture Inhomogeneity (Air Pocket)

Compensator Target Area Aperture Inhomogeneity (Air Pocket)

Compensator Target Area Aperture Inhomogeneity (Air Pocket)

Compensator Target Area Aperture Inhomogeneity (Air Pocket)

Smearing Radius

Compensator Target Area Aperture Inhomogeneity (Air Pocket)

Sacrificing distal conformity to ensure you have enough range (and Modulation) to cover the target Accounts for the fact that treatment path lengths may be different than planned path lengths due to set-up errors. Can easily be built into compensator design Not directly accounted for in PBS

The concept of smearing is used in compensator based proton therapy to account for : a) Possible compensator thickness errors generated by the milling process b) Inaccurate stopping power data of compensator materials c) Daily patient set-up uncertainties and possible movement of anatomical inhomogeneities during treatment d) All of the above

Patch Field Patch Line OAR Through Beam Tumor

Through Beam OAR Tumor Patch Field

Through Beam Tumor Match Field OAR Match Line

CTV GTV Patient ITV PTV = ITV + SM

Patient ITV PTV = ITV + SM

Patient PTV = ITV + SM

But. What about Range Uncertainties

Depends who you ask Paganetti, Phys. Med Biol (57), 2012

Moyers, Medical Dosimetry(35), 2010

Yang, Phys. Med. Biol, (57) 2012

Paganetti, Phys. Med Biol (57), 2012

Physical Distance (cm) Radiobiological Depth (WET)

Why is the standard PTV concept NOT fully applicable to proton therapy? a) Targets treated with protons tend to have no setup and intra-fraction changes in the target volume. b) The use of smearing negates the need for lateral margins in proton therapy. c) For protons, distal and proximal margins around the target are required to account for range uncertainties which are not accurately achieved using a standard PTV. d) None of the above.

Conversion from HU to RSP has inherent problems Noise Beam hardening Trying to make our CT scanner a spectrometer Two tissues can have same HU but different RSP Anything not natural can have large errors. Contrast Fillings Implants

MVCT Proton activation (PET/SPECT) Tomography Prompt Gamma verification Proton Tomography / radiography

No Compensator With Compensator

PBS With Compensator

OAR < 100% of Dose 100% of Dose

OAR < 100% of Dose 100% of Dose

OAR < 100% of Dose 100% of Dose

OAR < 100% of Dose 100% of Dose

Robustness analysis Move individual fields and recalculate Mimic Set-up errors Re-assign shifted HU conversion curves and recalculate Mimic HU conversion errors Move Target structures and recalculate Mimic smearing

The true benefit of proton is in the difference in integral dose. Make the best of this!!

Faster layer switching Smaller and variable Spot Size Better understanding of Range Uncertainties Robustness tools for evaluations, probability DVH Robustness penalties included in optimization Robustness optimizations using in 4-D evaluations Streamlined Verification CT/plans Motivation to build strong proton protocols