Title: Front End Studies International Design Study
1Front End StudiesInternational Design Study
Muon Collider
- David Neuffer
- December 2009
2Outline
- Front End for the Neutrino Factory/MC
- Concepts developed during study 2A
- Concern on Vrf as function of Bsol
- 200MHz, 10 MV/m B 2T
- Variations
- Need baseline design for IDS
- need baseline for engineering study
- updated version to match IDS
- lower fields medium bunch length
3Plan for IDS
- Need one design likely to work for Vrf/B-field
- rf studies are likely to be inconclusive
- B1.25T V 10MV/m is very likely to work
- B 2T V 15 MV/m should work with Be
- Hold review to endorse a potential design for IDS
- likely to be acceptable (Vrf/B-field)
- April 2010 ?
- Use reviewed design as basis for IDS engineering
study
4Solutions for possible rf cavity limitations
- Potential strategies
- Use lower fields (V, B)
- 10MV/m at 1.5T?
- Use non-B constant lattices
- alternating solenoid
- Magnetically insulated cavities
- Is it really better ???
- Alternating solenoid is similar to magnetically
insulated lattice - Shielded rf lattices
- low B-field throughout rf
- Use gas-filled rf cavities
- same gradient with/without fields
- but electron effects?
- Use Be Cavities
- should have better B/ Vrf
5Shielded rf cooling channel (C. Rogers)
- Lattice that keeps B small within rf cavities
- Iron placed around coils
- B lt 0.25T at rf
- Problems
- rf occupancy 1/3
- larger ß (1m)
- tranverse acceptance
- Still has fair cooling
- increases µ/p by 1.7
3m
rf cavity
6Baseline IDS candidate
- ISS study based on nB 18 ( 280 MeV/c to 154
MeV/c) - 1.75T, 12MV/m
- Reference -shorter has nB 10 ( 280 MeV/c to 154
MeV/c) - slightly higher fields (2T, 15MV/m)
- Looking for candidate variation for IDS
- developing intermediate case, with a bit weaker
fields
7Recent Studies on Lower Fields
- Adequate acceptance can be obtained by reducing
magnetic fields and gradients - B -gt 1.25T, V -gt 10 MV/m ??
- (10MV/m is 7MV/m real estate gradient could use
7MV/m if space is filled.) - Reduced B, V are relatively certain to work.
- Cost optimum?
- B1.5T ?, 12MV/m
0.75T, 14MV/m
8Look at performance if Vrf is reduced
- Muons per 10 8-GeV protons
Cooler/ Rotator 10 12 14 15 17 18 MV/m
10 0.35 (0.63) 0.55 (0.67) 0.66 0.73
12 0.57 (0.72) 0.754 0.77 0.80
14 0.776 0.80 0.82 0.84
15 0.81 0.85 0.88 0.84
(0.65cm) (0.8cm)
B2T (B1.25T 5 worse) - B 1.5T 5 better
Variation is not strong more rf still means more
muons
9Front End ReOptimization
- Change reference B-field to 1.5T
- constant B to end of rotator
- Redoing nB 12 example
- A bit longer than nB 10
- optimize with lower fields
- Vrf lt 12 MV/m
- Will see if we can get better optimum
10High-frequency Buncher and f-E Rotator
- Drift (p?µ)
- Adiabatically bunch beam first (weak 320 to 232
MHz rf) - F-E rotate bunches align bunches to equal P
(233MeV/c) - 232 to 202 MHz, 12MV/m
- Cool beam 201.25MHz
11Parameters of candidate release
- Initial drift from target to buncher is 79.6m
- 18.9m (adiabatic 20T to 1.5T solenoid)
- 60.7m (1.5T solenoid)
- Buncher rf 33m
- 320 ? 232 MHz
- 0 ? 9 MV/m (2/3 occupancy)
- B1.5T
- Rotator rf -42m
- 232 ? 202 MHz
- 12 MV/m (2/3 occupancy)
- B1.5T
- Cooler (50 to 90m)
- ASOL lattice, P0 232MeV/c,
- Baseline has 15MV/m, 2 1.1 cm LiH absorbers /cell
0.08
µ/p
cooling
0.00
12progression through system
z 1m
80m
156m
215m
112m
13 NF Release Candidate
- Front End a bit longer than short example
- 50m shorter than ISS, however
- gradients no greater than ISS baseline
- slightly better performance
66m bunch window
14How Long a Bunch Train for IDS?
- ISS study alotted space for 80 bunches (120m long
train) - 80m or 54 bunches is probably plenty
Study 2A
80m
-20
100
nB 10
50m
40
-30
15Bunch train length
- Within IDS design could reduce bunch train to
80m (52 bunches) - very little mu loss
- With shorter front end, could reduce that to 50m
or less - For Collider scenario 12 best bunches, (18m)
contains 70 of muons - Reserving 80m for bunch trains should be adequate
for IDS
Study 2A
20m
16B0 1.5T, nB 12 RC
- Muons per 10 8-GeV protons (Atlt 0.03, ALlt0.02)
Cooler/ Rotator 10 12 14 15 16 18 MV/m
10 0.35 (0.63) 0.55 (0.67) 0.66 0.73
12 0.57 (0.72) 0.754 0.84 0.77 0.856 0.88 0.80
14 0.776 0.80 0.84
15 0.81 0.85 0.84
(0.65cm) (0.8cm) 1.0cm 1.1cm 1.15
Black are old nB 10 example new version is
Green
17Varying Buncher/Rotator Voltage
- Vary buncher/rotator gradients from baseline to
explore sensitivity to gradient limits. - same baseline cooling channel (16MV/m, 1.15cm
LiH) - 15 MV/m -gt 1.1cm Li H
- Somewhat less sensitive than previous
Buncher / Rotator 0/0 3/6 4/7 5/8 6/9 7/10 8/11 9/12
µ/8GeVp at 240m (10) .136 .508 .686 .753 .797 .800 .831 .857
10/ 13 11/ 14
.821 .839
18rf requirements
- Buncher
- 319.63, 305.56, 293.93,285.46, 278.59, 272.05,
265.80, 259.83, 254.13, 248.67, 243.44, 238.42,
233.61 (13 f) - 100MV total
- Rotator
- 230.19, 226.13, 222.59, 219.48, 216.76,
214.37,212.28, 210.46,208.64, 206.90,
205.49,204.25, 203.26, 202.63,202.33 (15 f) - 336MV total
- Cooler
- 201.25MHz up to 75m 750MV
19Plans etc.
- Move toward realistic configuration
- More realistic B-field
- B 1.5T -gt coil-based fields
- add Be windows
- smaller number of rf frequencies
- Set up design for cost algorithm
- rf cavity design (pillbox, dielectric)
- rf power requirements
- Magnet design
- Continuing front end IDS design study
- C. Rogers, G. Prior, D. Neuffer, C. Yoshikawa, K.
Yonehara, Y. Alexahin, M. Popovic, Y. Torun, S.
Brooks, S. Berg, J. Gallardo - Fermilab meeting (July)
- Biweekly phone Conference
- Meeting at RAL
- December 14-18
- April at Fermilab (IDS meeting)
dielectric
20IDS - cost issues
21Study2B June 2004 scenario (ISS)
- Drift 110.7m
- Bunch -51m
- 12 rf freq., 110MV
- 330 MHz ? 230MHz
- ?-E Rotate 54m (416MV total)
- 15 rf freq. 230? 202 MHz
- P1280 , P2154 ?NV 18.032
- Match and cool (80m)
- 0.75 m cells, 0.02m LiH
- Captures both µ and µ-
- 0.2 µ/(24 GeV p)