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Berkeley Lab Generic Presentation

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Pre-accelerator (273 MeV/c ? 1.5 GeV) based on solenoid focusing ... Nonliner focusing at r = 20 cm for 1 m long solenoid with 25 cm aperture radius ... – PowerPoint PPT presentation

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Title: Berkeley Lab Generic Presentation


1
Beam Dynamics of Low Energy Muon Acceleration
Alex Bogacz Jefferson Lab
7-th International Workshop on Neutrino
Factories and Superbeams, LNF Frascati, June 24,
2005
2
Overview
  • FFAG acceleration below 5 GeV not cost effective
  • Dogbone RLA (3.5-pass) scheme based on 200MHz
    SRF
  • Pre-accelerator (273 MeV/c 1.5 GeV) based on
    solenoid focusing
  • Main Linac (1 GeV/pass) based on triplet focusing
  • Three droplet arcs with horizontal multi-pass
    separation
  • Longitudinal phase-space compression in the arcs
    (M45 and off-crest RF)
  • M45 and off-crest RF linac acceleration
  • Large (?2) transverse acceptance
  • Lattices linear optics, tracking studies,
    emittance preservation
  • multi-pass linac optics
  • tracking studies

3
Muon Acceleration Complex
  • Linear pre-accelerator (273 MeV/c 1.5 GeV)
  • Dogbone 3.5-pass RLA (1.5 5 GeV)
  • 5 10 GeV FFAG
  • 10 20 GeV FFAG

4
Dogbone RLA (3.5-pass) scheme
  • Linear pre-accelerator (273 MeV/c 1.5 GeV) -
    solenoid focusing
  • Main Linac (1 GeV/pass) - triplet focusing
  • Single magnet horizontal multi-pass separation
  • 3 Arcs based on the same strength of bending
    magnets ( 1 Tesla)

5
Initial beam emittance/acceptance
after the cooling channel at 273 MeV/c
6
Beam Parameters
7
Pre-accelerator Longitudinal dynamics
longitudinal acceptance, bucket height
energy profile along the linac
Dp/p?0.17or Df ?93 (200MHz)
8
Pre-accelerator Longitudinal acceptance
Phase space contours initial, half-way through
and at the end of acceleration contours defined
for particles at 2.5s (95 of particles contained
inside)
9
Linear Pre-accelerator Longitudinal dynamics,
tracking
10
soft-edge solenoid model
  • Zero aperture solenoid - ideal linear solenoid
    transfer matrix

Larmour wave number
11
soft-edge solenoid edge effect
  • Non-zero aperture - correction due to the finite
    length of the edge
  • It decreases the solenoid total focusing via
    the effective length of
  • It introduces axially symmetric edge focusing at
    each solenoid end
  • axially symmetric quadrupole

12
soft-edge solenoid nonlinear effects
  • Nonlinear focusing term DF O(r2) follows from
    the scalar potential
  • Scalar potential in a solenoid
  • Solenoid B-fields

13
soft-edge solenoid nonlinear effects
  • In tracking simulations the first nonlinear
    focusing term, DF O(r2) is also included
  • Nonliner focusing at r 20 cm for 1 m long
    solenoid with 25 cm aperture radius

14
Linear Pre-accelerator transverse emittance
15
Main Linac - multi-pass Optics
  • Focusing compromise strategy
  • focusing optimized for the half-pass (1.5-2 GeV)
    - 900 phase advance per cell
  • Uniform focusing restored in the second half of
    the first full-pass (2.5-3 GeV)

16
Main Linac - Multi-pass Optics (lower passes)
1.5-2 GeV
2-3 GeV
17
Main Linac - Multi-pass Optics (higher passes )
3-4 GeV
4-5 GeV
18
Main Linac - Multi-pass phase advance slip
2-3 GeV
3-4 GeV
19
Main Linac - the half-pass (1.5-2 GeV)
longitudinal tracking
20
Main Linac - transverse emittance (tracking)
the half-pass 1.5-2 GeV
21
Arc Optics - beam transport choices
  • Principle of uniform focusing periodicity (900)
    cancellation of chromatic effects
  • Single dipole (horizontal) separation of
    multi-pass beams in RLA
  • No need to maintain achromatic Spreaders/Recombine
    rs
  • Compact Spreaders/Recombiners minimized
    emittance dilution
  • SC dipoles and quads (triplets) in RLA (1 Tesla
    dipoles/1 Tesla quads)
  • Requirement of high periodicity and smooth
    transition between different kinds of optics,
    linac-spreader-arc-recombiner-linac

22
Droplet return (600 out - 3000 in - 600 out)
  • arc footprint

23
Droplet arc Optics building blocks
  • inward and outward cells, missing dipole cell

24
Chromatic properties of the periodic cell
  • Dp/p?0.07

25
Droplet Arc Optics (Spreader and Transition) -
Arc 1
Quads Lcm GkG/cm D 68 -0.32 F 125 0.32
Dipoles Lcm BkG 150 7.8
26
Arc 1 Longitudinal dynamics (tracking)
27
Arc 1 Transverse emittance (tracking)
28
Arc 2 Optics
29
Summary
  • Lattice for 3.5-pass, 5 GeV, RLA based on 200MHz
    SRF - linear optics
  • Pre-accelerator, three styles of cryo-modules
  • Proof-of-principle Arc optics lattice - further
    longitudinal compression in the Arcs, with M56
    3 m
  • multi-pass linac optics
  • compact Spr/Rec
  • matched periodicity (betatron phase advance per
    cell) between linacs and Arcs
  • Future work
  • Emittance preservation scheme - nonlinear
    corrections in the Arcs
  • Chromatic corrections in the Arcs to effectively
    restore longitudinal space linearity (via three
    families of sextupoles)
  • Emittance preservation checked independently by
    ICOOL
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