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NON-SCALING FFAGs: questions needing answers. Andy Wolski The Cockcroft Institute, and the University of Liverpool Department of Physics. BASROC-CONFORM Project Open Day Daresbury Laboratory 11 May 2009. Setting The Scene. Project Overview.
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NON-SCALING FFAGs:questions needing answers Andy Wolski The Cockcroft Institute,and the University of Liverpool Department of Physics. BASROC-CONFORM Project Open Day Daresbury Laboratory 11 May 2009
Project Overview BASROC (The British Accelerator Science and Radiation Oncology Consortium, BASROC) FFAG s --- Reduced size, cost and complexity Ns-FFAG --- Even simpler and more compact • CONFORM project ( COnstruction of a Non-scaling FFAG for Oncology, Research, and Medicine ) • 4 year projectApril 2007 – March 2011 • 3 parts to the project • EMMA design and construction~ £6.5m Electron Model for Many Applications (EMMA) • PAMELA design study • Applications study isosceles
Proton & Carbon Therapy • Neutrino Factory Applications of ns-FFAGs High power proton driver • Sub-critical Thorium Reactor • Dedicated Muon Source
WHY FFAGs? 70 MeV ISIS Synchrotron ACCEL Proton Cyclotron • LINACs • Use the RF only once, too expensive • long • Synchrotrons • Ramp the magnets and the RF • Complex to operate • Acceleration is slow • Repetition rates are 1-100 Hz • Cyclotrons • Very large complex magnets • Inflexible extraction energy
Comparison Y. Mori – EPAC 06
Scaling FFAGs • They can be used to accelerate protons, electrons, muons and ions • They can be rapidly cycled, much faster than a synchrotron (Fixed Fields) • They have a large acceptance for a particle beam, much bigger than a synchrotron • They have the possibility of both large average and large peak beam currents • Beam can be extracted at a number of energies
Characteristics of Scaling FFAGs • Fixed tunes • Focusing strength constant with energy • Constant Betatron Tunes • Fixed orbit shape (largely increases with radius) • Large magnets • Large variation in time of flight • Changing RF frequency with Energy
Non-Scaling FFAGs Scaling FFAG Magnet Breaks the scaling requirement More compact orbits ~ X 10 reduction in magnet aperture Betatron tunes vary with acceleration Parabolic variation of time of flight with energy
Betatron Tunes & Resonance Crossing • Crossing resonances • Beam blowup • Beam loss • Can mitigate the effects of resonance crossing by:- • Fast Acceleration • Linear magnets (avoids driving strong high order resonances) • Or nonlinear magnets (avoids crossing resonances) • Highly periodic, symmetrical machine (many identical cells) • Tight tolerances on magnet errors dG/G <2x10-4 Can we cross resonances safely?
Revolution Period Varies with Energy • Three options for acceleration: • Asynchronous (highly relativistic) • Fixed rffrequency • Simplifies rf system, but leads tocomplicated longitudinal dynamics • “Normal” Synchronous • RF frequency and phase synchronisedwith time of flight. • Simplifies longitudinal dynamics, but requireshigh bandwidth cavities, with complicatedcontrols. • Harmonic Jump • Fixed rffrequency • Voltage and or phase maybe variable Can we accelerate?
Questions? How do we produce a compact lattice of linear magnets? How do we make it highly symmetric ? Does it have acceptance required for large emittance & high intensity beams? Can we fit all the accelerator components in this lattice? Can we inject and extract from a high compact , symmetric lattice? Is the dynamics in these accelerators as predicted by codes & simulation?