Notes
Slide Show
Outline
1
Context of the Neutrino Factory
  • Neutrino factory (2018)
    • 4MW proton driver
    • p+ ŕ p+ ŕ m+ ŕ e+nenm
  • Linear e+e− collider (2014/5)
    • Leptons at 0.4 to 1TeV
  • Muon collider (2023)
    • p+ ŕ p+,p− ŕ m+,m− ŕ
    • Multi-TeV lepton collision
  • and others…
2
Pion Capture and Muon Front-End
3
Muon1 Particle Tracking Code
  • Nonlinear 3-dimensional simulation
    • PARMILA was being used before
  • Uses realistic initial p+ distribution
    • Monté-Carlo simulation by Paul Drumm
  • Particle decays with momentum kicks
  • Solenoid end-fields included
  • OPERA-3d field maps used for FFAG-like magnets in chicane (Mike Harold)


4
Decay Channel Lattice
  • 12 parameters
    • Solenoids alternated in field strength and narrowed according to a pattern
  • 137 parameters
    • Varied everything individually
5
Improved Transmission
  • Decay channel:
    • Original design: 3.1% m+ out per p+ from rod
    • 12-parameter optimisation ŕ 6.5% m+/p+
      • 1.88% through chicane
    • 137 parameters ŕ 9.6% m+/p+
      • 2.24% through chicane
  • Re-optimised for chicane transmission:
    • Original design got 1.13%
    • 12 parameters ŕ 1.93%
    • 137 parameters ŕ 2.41%
6
Optimised Design for the Decay Channel (137 parameters)
7
Optimiser Architecture
  • How do you optimise in 137-dimensional space?
    • Hard to calculate gradient due to stochastic noise
    • Use genetic algorithm
      • Random designs
      • Mutation
      • Interpolation
      • Crossover

  • How do you run 3`700`000 simulations?
    • Distributed computing
    • Internet-based / FTP
    • ~130 users active in last week
      • >75`000 results sent in
    • Periodically exchange sample results file
8
Why did it make all the solenoid fields have the same sign?
  • Original design had alternating (FODO) solenoids
  • Optimiser independently chose a FOFO lattice
  • Has to do with the stability of off-energy particles
9
Design Optimised for Transmission Through Chicane
  • Nontrivial optimum found
  • Preferred length?
  • Narrowing can only be due to nonlinear end-fields
10
Recent Work on Losses
  • Muon1 modified to count lost particle energies
  • For a 4MW p+ beam:
    • 35kW deposited in S1 (r=10cm)
    • Large >1kW amounts deposited up to S5
  • Added “collimators” to the simulation
    • Decreases losses to 10’s of watts in all but S1 and S2
    • S1 needs enlarging to accommodate an entire Larmor rotation
  • Consistent target-area layout is needed
11
New Design with Muon Cooling
  • Decay channel (as before)
  • 31.4MHz RF phase rotation
    • Reduces energy spread from 190±70 to ±23MeV
  • Cooling ring (20 turns)
    • Uses H2(l) or graphite absorbers
    • Cooling in all 3 planes
    • 16% emittance loss per turn?