1 / 37

Alex Bogacz

Muon Acceleration for Neutrino Factory and Beyond. Alex Bogacz. Overview. Accelerator Topologies: ‘Racetrack vs Dogbone ’ Muon Acceleration for 5 GeV Neutrino Factory Linac + ‘ Dogbone ’ RLA: Beam Dynamics Issues Full bucket acceleration, Longitudinal compression

rmunoz
Download Presentation

Alex Bogacz

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Muon Acceleration for Neutrino Factory and Beyond Alex Bogacz

  2. Overview • Accelerator Topologies: ‘Racetrack vs Dogbone’ • Muon Acceleration for 5 GeV Neutrino Factory • Linac + ‘Dogbone’ RLA: Beam Dynamics Issues • Full bucket acceleration, Longitudinal compression • Longitudinal RF frequency shift: Matching chicane to accommodate μ± • Transverse Optics: Bi-sectedlinacs + ‘Droplet’ Arcs • Extending accelerator complex to 63 GeV Higgs Factory • Dogbone RLA with FFAG-like Arcs • Proof-of-Concept Optics • Demonstration Experiment: JEMMRLA Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  3. Accelerator Topologies ΔE/2 ΔE ΔE/2 ΔE/2 ΔE/2 ΔE Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  4. ‘Racetrack’ vs ‘Dogbone’ RLA ΔE/2 1.5ΔE ΔE/2 ΔE 3 ΔE • Twice the acceleration efficiency • Better separation of passes • Simultaneous acceleration of both charge species • Linac traversed in both direction ⇨ bi-sectedlinac optics Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  5. Linac and RLA to 5 GeV 255 MeV/c 160 m 1.25 GeV 5 GeV 70 m 840 MeV/pass Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  6. 5 5 BETA_X&Y[m] 20 20 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 160 Size_Y[cm] Size_X[cm] 0 0 0 Ax_bet Ay_bet Ax_disp Ay_disp 160 Initial 325 MHz Linac- Transverse Acceptance p = 255 MeV/c 1250 MeV beta functions Aacc= 20 MV/m f = 325 MHz 22 short cryos (2.5 meter, 2-cell cavity) 30 medium cryos (3.5 meter 4-cell cavity) 2.5 s beam envelope eN= 20 mm rad • x,y= 2.3 m • g = 2.1 • a = 15 cm eN= (2.5)2×eN_rms Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  7. 5 5 BETA_X&Y[m] 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 160 Initial Linac – Longitudinal Matching p = 255 MeV/c 1250 MeV beta functions Aacc= 20 MV/m f = 325 MHz Total RF installed: 1.513 GV 22 short cryos (2.5 meter, 2-cell cavity) 30 medium cryos (3.5 meter 4-cell cavity) Cavity off crest Synchrotron Tune Energy Bucket Area Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  8. 5 5 BETA_X&Y[m] 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 160 Initial Linac – Longitudinal Acceptance 1250 MeV p = 255 MeV/c beta functions Aacc= 20 MV/m f = 325 MHz Total RF installed: 1.513 GV 22 short cryos (2.5 meter, 2-cell cavity) 30 medium cryos (3.5 meter 4-cell cavity) Initial acceptance 150 mm (blue) Longitudinal compression Longitudinal acceptance eLong= 150 mm Dp/prms = 0.112 Dzrms = 10.3 cm eLong= (2.5)2×eLong_rms Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  9. RLA to 5 GeV 1.25 GeV 5 GeV 70 m 840 MeV/pass 650 MHz Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  10. 5 5 BETA_X&Y[m] DISP_X&Y[m] 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 240 325 MHz – 650 MHz Transition 1.25 GeV p = 255 MeV/c A325 MHz= 20 MV/m A650 MHz= 25 MV/m beta functions 325 MHz linac 650 MHz linac μ±time structure RF bucket Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  11. 2 20 BETA_X&Y[m] DISP_X&Y[m] -2 0 0 BETA_X BETA_Y DISP_X DISP_Y 15.89 2 20 BETA_X&Y[m] DISP_X&Y[m] -2 0 0 BETA_X BETA_Y DISP_X DISP_Y 16.12 Delay/Compression Chicane q q Dz q q 5 free parameters needed to match: 2 betas + 2 alphas + disp. q q Q2 Q3 Q4 Q3 Q1 Q2 Q1 Q0 Q0 Q’3 Q’3 Q’0 Q’2 Q’0 Q’1 Q’1 Q’4 Q’2 Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  12. 2 15 BETA_X&Y[m] DISP_X&Y[m] -2 0 0 BETA_X BETA_Y DISP_X DISP_Y 173.953 Longitudinal Compression with M56 Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  13. RLA to 5 GeV 1.25 GeV 5 GeV 70 m 840 MeV/pass 650 MHz Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  14. Bi-sectedLinac Optics 5 15 BETA_X&Y[m] DISP_X&Y[m] 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 35 5 15 BETA_X&Y[m] DISP_X&Y[m] 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 70 ‘half pass’ , 1250-1625 MeV initial phase adv/cell 90 deg. scaling quads with energy quad gradient 4meter 90 deg. FODO cells 25 MV/m, 650 MHz, 2×4-cell cavity 1-pass, 1625-2475 MeV mirror symmetric quads in the linac quad gradient Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  15. 5 30 BETA_X&Y[m] DISP_X&Y[m] 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 315 Multi-pass Linac Optics bx = 13.0 m by = 14.4 m ax=-1.2ay=1.5 bx = 7.9 m by = 8.7 m ax=-0.8ay=1.3 Arc 2 Arc 3 Arc 4 Arc 1 bx = 6.3 m by = 7.9 m ax=-1.2ay=1.3 bx,y → bx,y axy → - axy bx = 3.2 m by = 6.0 m ax=-1.1ay=1.5 bx,y → bx,y axy → - axy bx,y → bx,y axy → - axy bx,y → bx,y axy → - axy 4.175 GeV 1.25 GeV 1.625 GeV 2.475 GeV 3.325 GeV 5.025 GeV Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  16. Arc 1 and Arc 3 top view 1.625 GeV 3.325 GeV side view 1.625 GeV  1 m 3.325 GeV Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  17. Arc 1 and 3 – Optics 3 20 BETA_X&Y[m] DISP_X&Y[m] -3 0 0 BETA_X BETA_Y DISP_X DISP_Y 113.595 3 20 BETA_X&Y[m] DISP_X&Y[m] -3 0 0 BETA_X BETA_Y DISP_X DISP_Y 143.611 Arc 1 1.625 GeV 6 m cells 1 m dipoles 2 vertical steps 2 vertical steps Arc 3 3.325 GeV 8 m cells 2 m dipoles Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  18. Switchyard - Arc 1 and 3 1.625 GeV 3.325 GeV 1.625 GeV Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  19. Future Muon Facilities -Muon Acceleration n to Homestake Neutrino Factory LBNE Higgs Factory RLA to 63 GeV NF Decay Ring Linac + RLA to 5 GeV Project XStage III Project XStage II Project XStage I J.-P. Delahaye, MASS (Muon Accelerator Staging Studies) Fermilab Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  20. Higgs Factory: 5-pass RLA 5-63 GeV 5GeV 28.2 GeV 16.6 GeV 63 GeV 51.4 GeV 39.8 GeV 829 m 11.6 GeV/pass Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  21. Multi-pass Arc Muon RLA 5GeV (m±) 63 GeV 11.6 GeV/pass Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  22. Single- vs Multi- pass Droplet Arcs top view 16.6 GeV 39.8 GeV side view 16.6 GeV  1 m 39.8 GeV Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  23. Super-Cell Optics for P2/P1 = 2 • Each arc is composed of symmetric super cells consisting of linear combined-function magnets (each bend: 2.50) P 2xP Proof-of Concept Experiment: JEMMRLA -Jlab Electron Model of Muon RLA q = 600 Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  24. Summary • 5 GeV Neutrino Factory based on multi-pass ‘Dogbone’ RLA • Linac (255 MeV -1.25 GeV) Longitudinal Dynamics • Delay/Compression Chicane - Transition from 325 to 650 MHz SRF • RLA Optics (1.25 - 5 GeV ) - 4 droplet Arcs and multi-pass linac • Optimized RLA scheme for Higgs Factory • RLA with multi-pass arcs • Proof-of-Concept experiments: JEMMRLA and CBETA Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  25. Thank you for your Attention!Questions? Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  26. Backup Slides Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  27. 0.4-1.5 GeVLinac – Transmission Transmission: 1.4% loss Muon decay: 5% loss Total loss: 6.4% Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  28. Beam Loading J.S. Berg J.-P. Delahaye stored energy in a cavity: fractional reduction in the cavity voltage : RF gradient G defined as: fractional voltage reduction: Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  29. Multi-pass Linac – Bisected Optics E = 5-63 GeV Arc 2 Arc 1 Linac pass-1 Linac pass-2 Linac pass-3 RF f[MHz] cells/cavity Grad [MV/m] phase [deg] 650 5 25 22 Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  30. Arc Optics – Longitudinal Distortion 15 0.3 BETA_X&Y[m] DISP_X&Y[m] -0.3 0 303 BETA_X BETA_Y DISP_X DISP_Y 402.975 0 BETA_X BETA_Y DISP_X DISP_Y 100 15 0.3 BETA_X&Y[m] DISP_X&Y[m] -0.3 0 0 BETA_X BETA_Y DISP_X 3.34 E = 24 GeV M56 = -66.7 cm 2 half cells 15 cells out 2 half cells 2 empty cells 15 cells out 83 cells in 2 empty cells 900 FODO Quads L[cm] G[kG/cm] qF 80 10.2924 qD 80 -10.2788 Dipoles L[cm] B[kG] bend angle [deg] 50.00 49.3116 1.7647 Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  31. 300 60 C = 117.6 m Two-pass Arc Layout • Simple closing of arc geometry when using similar super cells • 1.2 / 2.4 GeV/c arc design used as an illustration can be scaled/optimized for higher energies preserving the factor of 2 momentum ratio of the two passes • Droplet arc: • 60 outward bend • 300 inward bend • 60 outward bend Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  32. ‘Droplet’ Arc - Spreader/Recombiner • First few magnets of the super cell have dipole field component only, serving as Spreader/Recombiner * Trajectories are shown to scale Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  33. A pair of 2-pass Arcs - Switchyard • Lower momentum arc is the most challenging because of the highest momentum ratio; have a solution but still plenty of room for optimization * Trajectories are shown to scale Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  34. Vertical Bypass Concept • 3xP • 4xP Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  35. ‘Pulsed’ quad Dogbone RLA 3 GeV 33 GeV 4 GeV/pass • Quad pulse would assume 500 Hz cycle ramp with the top pole field of 1 Tesla. • Equivalent to: maximum quad gradient of Gmax =2 kGauss/cm (5 cm bore radius) ramped over t = 10-3 sec from the initial gradient of G0 =0.1 kGauss/cm (required by 900 phase advance/cell FODO structure at 3 GeV) G8 =13 G0 = 1.3 kGauss/cm • These parameters are based on similar applications for ramping corrector magnets such as the new ones for the Fermilab Booster Synchrotron that have 1 kHz capability Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  36. 100 5 BETA_X&Y[m] DISP_X&Y[m] 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 254.651 100 5 DISP_X&Y[m] BETA_X&Y[m] 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 254.651 ‘Fixed’ vs ‘Pulsed’ linac Optics (8-pass) Fixed Pulsed Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

  37. 120 5 BETA_X&Y[m] DISP_X&Y[m] 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 254.651 5 120 BETA_X&Y[m] DISP_X&Y[m] 0 0 0 BETA_X BETA_Y DISP_X DISP_Y 254.651 ‘Fixed’ vs ‘Pulsed’ linac Optics (12-pass) Fixed Pulsed Muon Collider Workshop, Padua, Italy, July 1 - 3, 2018

More Related