The Particle Therapy Cancer Research Institute is a member of Introduction to Proton Therapy JAI Octoberfest, 3 rd October 2014 Claire Timlin Particle.

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Presentation transcript:

The Particle Therapy Cancer Research Institute is a member of Introduction to Proton Therapy JAI Octoberfest, 3 rd October 2014 Claire Timlin Particle Therapy Cancer Research Institute, University of Oxford

Introduction to Radiotherapy and Proton Therapy 3/10/2014 2

The Evolution of External Beam Radiation Therapy High resolution IGRT Multileaf Collimator Dynamic MLC and IMRT 1950’s 1970’s 1980’s 1990’s 2000’s? Cerrobend Blocks Electron Therapy FunctionalImaging The First Cobalt Therapy Unit and Clinac Computerized 3D CT Treatment Planning Standard Collimator Particle Therapy Slide courtesy of Prof. Gillies McKenna 3/10/2014 3

Goal of RT Radiation Induced Toxicity: – Central Nervous System: blindness, deafness, paralysis, confusion, dementia – Bowel: colostomy, chronic bleeding. – Lung: shortness of breath, pneumonias – Kidney: renal failure and hypertension – Reproductive organs: sterility – Everywhere: severe scarring in medium to high dose regions, possible increase in induced cancers in low-medium dose regions 4 3/10/2014 Maximise Tumour Dose Minimise Normal Tissue Dose

Photons/X-rays dose deposition Depth-dose curve – single beam Multiple Beams: Reduced dose to organs at risk – Fewer complications Increased tumour dose – Higher probability of tumour control However: – Large volumes of low-intermediate dose RT dose plan – multiple beams beam 3/10/2014 5

History of Proton Therapy 3/10/ : Therapy proposed - Robert R. Wilson, Harvard Physics 1955: 1 st Proton Therapy - Lawrence Tobias University of California, Berkeley : Single dose irradiation of benign CNS lesions - Uppsala, MGH, St Petersburg, Moscow 6

The Bragg Peak 3/10/ Components of the proton depth dose curve: – Bethe-Bloch formula Coulomb interactions with atomic electrons – Scattering, energy spread and interactions with atomic nuclei Illustrations from M. Goitein “Radiation Oncology: A Physicist’s-Eye View” © Springer, 2007 Dose Depth

Proton dose deposition Incident energy is modulated to form Spread Out Bragg Peak the cover the tumour Unnecessary dose 3/10/ The Daily Telegraph Australia

     With Protons Medulloblastoma in a Child 3/10/ With X-rays

Courtesy T. Yock, N. Tarbell, J. Adams Orbital Rhabdomyosarcoma 3/10/ X-Rays Protons/Ions

Proton Therapy in Action Anaplastic Ependymoma Brain Tumour /10/ CPC, Friedmann, NEJM, 350:494, 2004 Pre-treatment During-treatment Post-treatment Slide courtesy of Prof. Gillies McKenna

Number of treatment centres worldwide > 93,000 patients > 10,000 patients Protons: 40 operational, ~ 40 in development carbon: 8 operational, 4 in development 3/10/

Proton Therapy Centre World Map 3/10/ Protons - low energy Protons – high energy Carbons

Proton Therapy Centre Europe Map 3/10/ Protons - low energy Protons – high energy Carbons

Many more in the planning stages…. 3/10/

Proton Therapy in UK 3/10/ Clatterbridge – 1989: First hospital based proton therapy at Clatterbridge, near Liverpool – ~2500 patients with ocular melanoma; local control ~97%. – Targets the cancer – Avoids key parts of eye (optic nerve, macula, lens) Simon to talk about UCLH and Manchester….

Production and Delivery of Medical Proton Beams 3/10/

Beam Production and Acceleration 3/10/ Ion source – Plasma accelerated in electric field Acceleration – Cyclotron Fixed magnetic field Fixed energy Constant frequency – Synchrotron Fixed radius Variable magnetic field Synchronous frequency – Future accelerators that do the job better? HIT, Germany

Beam Transport 3/10/ Gantries Fixed Beams Clinical Indications Flexibility Space Cost

Courtesy of T. Lomax, PSI, Switzerland. Beam Delivery - Scattering 3/10/

Beam Delivery - Scanning 3/10/ Exploiting depth control Exploiting charge Beam direction Patient Target

Some challenges in Proton Therapy 3/10/ Acceleration and Beam transport: – Faster spot scanning – More compact accelerators and gantries – Beam switching and splitting Uncertainty in planned vs. delivered dose: – Range uncertainties – Relative biological effectiveness Treatment delivery – Organ motion – Hypo-fractionation Which clinical indications? – Cost-effectiveness – Ethics Lack of data and models to predict late effects e.g. second cancers

Some possible solutions 3/10/ Accelerator development Radiobiological modelling and experiments Advanced treatment planning and delivery techniques – Novel, high resolution, minimally damaging imaging – Dose validation/online dosimetry Consistent data recording and data sharing Clinical studies with long-term follow-up

University of Oxford’s hope for Protons 3/10/

Early Stage Cancer Patient Molecular Stratification Precision Cancer Medicine Institute Big Data Institute Big Data Institute Oxford Cancer Imaging Centre Structural Genomics Consortium Population Health Science Experimental Cancer Medicine Centre Increased Cures Target Discovery Institute Courtesy of Gillies McKenna Targeted cancer treatment pathway 3/10/

Precision Cancer Medicine 3/10/  Physically Targeted  Robotic Surgery  Proton Therapy  HIFU  Physiologically Targeted  Molecular Imaging  Molecularly Targeted  Deep Genomic Sequencing  Biomarker Driven  Biologically targeted Courtesy of Gillies McKenna

Oxford Precision Medicine Institute Genomics Particle Therapy Robotic Surgery Functional and Molecular Imaging Targeted Agents Courtesy of Gillies McKenna 3/10/

Molecular Imaging Nanotechnology Proton Therapy Robotics HIFU CT, MRI, PET Targeted Agents (CF 3 ) 180 Genomics Courtesy of Gillies McKenna The Evolution of Cancer Therapy 3/10/ Increased Effectiveness, Reduced Toxicity

3/10/ Thank you…. ……….any questions?

Extra Slides 3/10/

Induction and cell kill 3/10/ Induction Cell killing What is the form of the induction function? Linear, quadratic? Form of cell killing function known with some certainty at clinical energies, the parameters are tissue dependent and can have large uncertainties. Risk needs to be accurately modelled confirmed experimentally taken into account when deciding on the optimal treatment plan Probability of transforming a cell Probability of inducing a potentially malignant mutation Probability the cell survives

Second cancer risk IMRTIMPT 3/10/

Second cancer risk IMRTIMPT 3/10/

Cell LevelVoxel LevelPatient Level Multiscale, voxelised TCP calculation for GBM Cellularity Tumour microenvironment: P0 2 Genetic heterogeneity: Stem vs. non- stem Dose matrixStructure matrixPost treatment CCD Tumour recurrence time Clinical Data Number of fractions Radiobiological parameters e.g. ,  Treatment plan DICOM files Cell automaton model Pre-treatment clonogenic cell density (CCD) Predicted TCP 3/10/

Relative Biological Effectiveness 3/10/ Photons and protons (at clinical energies) have similar biological effects – Clinically a modifier (RBE) of 1.1 is applied to physical dose for protons For heavier ions (e.g. C) RBE has large uncertainties RBE needed* to calculate physical dose to administer to achieve prescribed biological dose *maybe there is a better way? New treatment regimes requiring new methods of optimisation?

RBE vs. Dose for Protons Paganetti et al.: Int. J. Radiat. Oncol. Biol. Phys. 2002; 53, 407 Where does the 1.1 come from? 3/10/