Title: Berkeley Lab Generic Presentation
1Beam Dynamics of Low Energy Muon Acceleration
Alex Bogacz Jefferson Lab
7-th International Workshop on Neutrino
Factories and Superbeams, LNF Frascati, June 24,
2005
2Overview
- 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
3Muon 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
4Dogbone 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)
5Initial beam emittance/acceptance
after the cooling channel at 273 MeV/c
6Beam Parameters
7Pre-accelerator Longitudinal dynamics
longitudinal acceptance, bucket height
energy profile along the linac
Dp/p?0.17or Df ?93 (200MHz)
8Pre-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)
9Linear Pre-accelerator Longitudinal dynamics,
tracking
10soft-edge solenoid model
- Zero aperture solenoid - ideal linear solenoid
transfer matrix
Larmour wave number
11soft-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
-
12soft-edge solenoid nonlinear effects
- Nonlinear focusing term DF O(r2) follows from
the scalar potential - Scalar potential in a solenoid
- Solenoid B-fields
13soft-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
14Linear Pre-accelerator transverse emittance
15Main 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)
16Main Linac - Multi-pass Optics (lower passes)
1.5-2 GeV
2-3 GeV
17Main Linac - Multi-pass Optics (higher passes )
3-4 GeV
4-5 GeV
18Main Linac - Multi-pass phase advance slip
2-3 GeV
3-4 GeV
19Main Linac - the half-pass (1.5-2 GeV)
longitudinal tracking
20Main Linac - transverse emittance (tracking)
the half-pass 1.5-2 GeV
21Arc 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)
23Droplet arc Optics building blocks
- inward and outward cells, missing dipole cell
24Chromatic properties of the periodic cell
25Droplet 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
26Arc 1 Longitudinal dynamics (tracking)
27Arc 1 Transverse emittance (tracking)
28Arc 2 Optics
29Summary
- 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