1. Part IV Applications

2. Prototype of Cancer therapy machine with proton 150 MeV FFAG as a prototype Commissioning to accelerate up to ~15 MeV is done. Tune survey

3. Requirements Accurate positioning –Irradiate a well defined 3-dimensional volume (and not outside.) Accurate dose –Dose at each point should be controlled with accuracy of 1%.

4. Broad beam method (Conventional) Final collimator Bolus Ridge filter Inevitable irradiation outside of the treatment field. Each patient needs his own shaped bolus.

5. Spot scanning method A small beam spot makes it possible to irradiate a well defined area. Non-uniform irradiation in the area is possible. Simultaneous dose measurement using supersonic waves.

6. Supersonic wave detector Reconstruction of irradiated volume in 3D space. Treatment volume Pulsed beam produces pulsed supersonic wave from irradiated position

7. Experiment (green) Calculation (red) Pressure of sound Detection of supersonic waves induced proton beam pulse

8. Disadvantage of spot scanning Sensitive to respiratory motion Organ motion during scanning should be suppressed. Beam irradiation time should be shortened much less than respiratory motion. Intensity of each pulsed beam should be accurately controlled.

9. Dream machine Small spot beam with variable extraction energy (pulse by pulse). –A beam is delivered to localized volume (no other places.) Beam intensity is well controlled (pulse by pulse). –Accurate dose distribution. High intensity (per pulse) pulsed beam. –Short irradiation time compared to respiratory motion. Pulsed beam with very high repetition frequency –Simultaneous dose measurement using supersonic waves. Small size, low cost, and easy operation.

10. FFAG as a medical accelerator Spot scanning with 1kHz or more repetition rate. Variable energy extraction, pulse by pulse. 1% level of does control in a pulse using beam chopper after ion source. High peak as well as high average current is available due to very rapid cycling and alternating gradient (strong) focusing. Small size, low cost, and easy operation.

11. Injector (Cyclotron) RF system Extraction beam line The system for Spot scanning 5m 150MeV FFAG - Overview Commissioning at East-Experimental hall of KEK-PS Schematic view of 150MeV FFAG Parameters

12. Design of the magnet pole Magnetic field in the center of the sector BL Gap is not exactly r k in low momentum region. Rogowski like patch is attached on focusing magnet. BL is adjusted instead of local B(  ).

13. with patch w/o patch Correction of magnet The design of the edge of the F-sector pole The final design of the poles with extension w/o extension BL-F/D ratio vs. radius Focusing sector Defocusing sector Unit : mm A comparison of F-sector magnetic field on the medium plane excursion

14. Before and after correction Tune excursion is reduced after correction. before after

15. Betatron tunes Betatron tunes by a beam simulation with final design of the magnet. Betatron tunes vs. mean radius integer resonance half integer resonance third resonance Tune diagram

16. Return Yoke Free Magnet “Return Yoke Free Magnet ” The return yoke of Focusing sector is removed. F Sector D Sector Shunt Φ F : Magnetic field in F Sector Φ D : Magnetic field in D Sector Φ S : Magnetic field in Shunt Yoke F coil D coil Space for the extraction

17. 150 MeV FFAG - Return Yoke Free Magnet 150 MeV FFAG magnet, the view from the center of the ring.

18. Measurements of magnetic field. Discrepancy (ΔB/B) Measurements of magnetic field with hole probe. The discrepancy between any two magnets is 0.3% at most. The alignment error of hole probe explained that discrepancy. Y=-35~+45cm 5cm step -15000 -10000 -5000 0 5000 10000 15000 20000 -120-100-80-60-40-20020 X (cm) Bz (Gauss) Magnetic Field (Bz) X Y D F D Defocus sector Focus sector Defocus sector Focus sector Magnet center

19. Chamber 2m 1.2m

20. alignment

21. Injector cyclotron and beam transport

22. Beam is circulating on April 25, 2003.

23. Beam position in first 3 turns Without (left) and with (right) injection bump ES MS

24. Commissioning with SAD demonstration

25. Circulating beam and its tune BPM raw data and its frequency

26. Tune of design and measurement calculation

27. Effects of neighboring components Fe next to magnets distorts closed orbit.

28. Tune shift by COD Tune is a function of COD.

29. acceleration

30. Goal of study Prototype machine (150MeV) is under commissioning. MA based RF cavity Yoke-free magnet Demonstration of 3D spot scanning

31. PRISM phase rotator To study muon rare decay, mono chromatic muons are necessary. Secondary particles produced by intense protons have large momentum spread. –Phase rotation to convert large dp/p and small dt to small dp/p and large dt. –5 turns in FFAG makes 1/4 synchrotron oscillation. PRISM specifications –Number of sector8 (or 10) –Radius5 m –Triplet sector –Acceptance10,000 pi mm-mrad

32. Physics goal of PRISM project

33.  -> e conversion in Muonic Atom

34. Phase rotation

35. PRISM layout

36. Simulation study with GEANT3.21

37. Phase rotation with two RF waveform

38. Momentum compression projected in horizontal plane

39. PRISM issues Large aperture RF core Large aperture kicker High repetition

40. FFAG for ADS Feasibility study of ADSR –Five year program from 2002 to 2006 Subjects –Accelerator technology Variable energy FFAG –Reactor technology Basic experiments for energy dependence of the reactor physics Hosted by Kyoto University Research Reactor Institute (KURRI)

41. What is ADSR? Accelerator driven Sub-critical Reactor Chain reaction is controlled by beam. accelerator Sub-critical reactor Target for generating neutrons

42. Accelerator driven sub-critical reactor (ADSR) Basic study of accelerator driven system. 3 stage FFAG –2.5 MeV spiral (ion beta) FFAG with induction cores –25 MeV radial (booster) FFAG with RF and flat gap –150 MeV radial (main) FFAG with RF and tapered gap Variable output energy become possible by –Variable k value at booster FFAG Orbit excursion should be the same to locate the same injection and extraction radius. Momentum ratio at main FFAG is constant. Magnetic strength is variable. Upgrade to 1 GeV system is considered.

43. Layout of ADSR FFAG

44. Neutrino factory Accelerate muons to 20 - 50 GeV/c Initial momentum is 0.3 - 1 GeV/c 3 or 4 FFAG cascade –0.3 - 1 GeV/c(0.3 - 1 GeV/c with nuon cooling) –1 - 3 GeV/c or1 - 4.5 GeV/c –3 - 10 GeV/c4.5 - 20 GeV/c –10 - 20 GeV/c JPARC 50 GeV Main Ring is a proton driver.

45. Neutrino factory with JPARC proton driver

46. Acceleration of muons No time to modulate RF frequency. 1 MV/m (ave.) RF voltage gives large longitudinal acceptance. From 10 to 20 GeV/c within 12 turns.

47. Issues Kicker Non scaling FFAG