bunched-beam phase rotation for a neutrino factory david neuffer, andreas van ginneken, daniel...
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![Page 1: Bunched-Beam Phase Rotation for a Neutrino Factory David Neuffer, Andreas Van Ginneken, Daniel Elvira Fermilab](https://reader035.vdocuments.mx/reader035/viewer/2022070400/56649f0c5503460f94c2059d/html5/thumbnails/1.jpg)
Bunched-Beam Phase Rotationfor a Neutrino Factory
David Neuffer,Andreas Van Ginneken, Daniel Elvira
Fermilab
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Outline Study I – II -Factory – feasible but too expensive
Remove Induction Linac Replace with High-Frequency Buncher and phase-energy rotation:
Capture beam in high-frequency buckets Reduce energy spread with high-frequency E rotation Inject into fixed-frequency cooling
Simulation and Optimization Simucool – adds transverse motion + some optimization DPGeant – fully realistic simulation; match into realistic cooling
Discussion Cost estimates ??? Future development
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Study 2 Costs …. “Cost” reduced by ~25% from Study I
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Induction Linac Technology•Study II scenario uses ~ 250m long induction linac to capture muons.• Cost is prohibitive
•Technology is difficult
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System Overview
Drift (100m) – decay and drift
Buncher (60m) 300187MHz, V 4.8 (z/L)2 MV Trap beam into string of ~200 MHz bunches
E Rotator(8.4m) 187MHz, V = 10 MV/m rotate string of bunches to ~ equal energies
Cooler (100m) 183MHz – ionization cooling
beam Drift Buncher
Rotator
Cooler
Overview of transport
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Longitudinal Motion Through System
Drift Bunch
E rotate Cool
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SIMUCOOL Beam at end of buncher
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Simucool-optimized buncher and fixed frequency E rotation
Obtains ~0.28 /p at end of buncher
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Simucool optimizations (AvG) Large statistics tracking code (SIMUCOOL) can be used
to reoptimize Buncher + E Rotation
Reoptimize baseline adiabatic buncher and fixed frequency E rotation (track rms bunches in each band) – Obtains ~0.3 /p (up from 0.25)
Change fixed-frequency to “vernier”; sets phase to N-1/2 wavelengths from first to last ref. bunch; maximizes E rotation - obtains ~0.35 /p
Retrack with ICOOL – similar results are obtained
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“Vernier”-optimized E rotation
Obtains ~0.34 /p at end of buncher
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Latest Optimizations A van Ginneken has completed a new set of
optimizations; changes some parameters Drift – reduced to ~76m Buncher parameters changed:
Reference energies: 64 MeV; 186MeV 20 bunches between reference energies 384233
MHz Linear ramp in voltage 0 to 6.5MV/m Still 60m long
Rotator changed “vernier” frequency (20 + ) wavelengths between
reference bunches (234220 MHz), 10MV/m Optimize on longitudinal bunch densities Best case has 0.16 Longer Rotator (~30m)
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System Components (new version)
Drift (80m) Buncher (60m) 380230 MHz, V 6.5 (z/L) MV/m E Rotator(30m) 230220 MHz, V = 10 MV/m Cooler (100m) ~220 MHz
beam Drift Buncher
Rotator
Cooler
Overview of capture transport
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Bunching and Rotation
Beam after drift plusadiabatic buncher – Beam is formed intostring of ~ 200MHz bunches
Beam after ~200MHz rf rotation;Beam is formed into string of equal-energy bunches;matched to cooling rf acceptance
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DPGeant simulations (D. Elvira) Fully “realistic” transverse and longitudinal
fields Magnetic fields formed by current coils Rf fields from pillbox cavities (within solenoidal coils
Studied varying number of different rf cavities in Buncher (60 (1/m) to 20 to 10) … 20 was “better”, 10
only a bit worse
Simulations of -E rotation
Will extend simulations + optimization through cooling channel
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Beam at end of drift
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Beam at end of Buncher
64.9 % of the particles survive at the end of the buncher
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DP Geant results – rf rotation
First rf rotation with DPGeant
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Hardware For Adiabatic Buncher
Transverse focussing (currently) B=1.25T solenoidal focusing R=0.30m transport for beam
Rf requirements: Buncher: ~300~200 MHz; 0.14.8MV/m
(60m)(initially 1 cavity every 1m; reduces frequency in 2-
4MHZ steps; 1-D and other early simulations indicate ~10 frequencies are sufficient (~10MHz intervals)
Rotator: 230220 MHz; 10MV/m (~10m)
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RF requirements for High-frequency buncher and phase rotation
Rf frequency Voltage (Quadratic to Linear ramp)
300 MHz 0.075 - 1 MV - 6m
290 MHz 0.675 - 4 MV - 6m
280 MHz 1.875 - 7 MV - 6m
270 MHz 3.675 - 10 MV - 6m
260 MHz 6.08 - 13 MV - 6m
250 MHz 9.08 - 16 MV - 6m
240 MHz 12.7 - 19 MV - 6m
230 MHz 16.9 - 22 MV - 6m
220 MHz 21.7 - 25 MV - 6m
210 MHz Buncher:
28 MV - 6m ( Total rf voltage: 101 to 145 MV)
200 MHz 100 MV (10m) - Rotator
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Rf Cost Estimate (Moretti)Frequency
Cavity length
Cavity Cost
Rf Power Total
300MHz 0.5 m 225 k$ 225 k$ 450k$
290 1 450 350 800
280 2 900 700 1600
270 2 900 1000 1900
260 2 900 1000 1900
250 2 900 1000 1900
240 2 900 1000 1900
230 3 1200 1500 2700
220 4 1400 1500 2900
210 5 1800 2000 3800
200 10 3800 4200 8000
33.5m 13375 14475 27850k$
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Transport requirements Baseline example has 1.25 T solenoid for entire
transport (drift + buncher + rf rotation) (~170m)
Uncooled -beam requires 30cm radius transport (100m drift with 30cm IR – 1.25T)
In simulations, solenoid coils are wrapped outside rf cavities. (~70m 1.25T magnet with 65cm IR)
FODO (quad) transport could also be used …
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Cost of Solenoid (PDG handbook)
Stored Energy:
Cost:
Combine 2 solenoids: 3.5 + 7.9 = 11.4 M$ Multiply by ~2 ~20 M$ ?
(D. Summers can do Al solenoids for ~10 M$)
LRB2
E 22
0
662.0)MJ(E532.0Cost
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Cost of magnets (M. Green)
100m drift: 11.9 M$ (based on study 2)
Buncher and phase rotation: 26 M$ (study 2) Cryosystem: 1.5M$; Power supplies 0.5M$
Total Magnet System : 40M$
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$$ Cost Savings ?? High Frequency -E Rotation replaces Study 2:
Decay length (20m, 5M$) Induction Linacs + minicool (350m, 320M$) Buncher (50m, 70M$)
Replaces with: Drift (100m) Buncher (60m) Rf Rotator (10m) Rf cost =30M$; magnet cost =40M$ Conv. Fac. 10M$
Misc. 10M$ ……
Back of the envelope:(400M$ ?? 100M$ )
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Summary High-frequency Buncher and E Rotation
simpler and cheaper than induction linac system Performance probably not as good as study 2,
But System will capture both signs (+, -)
To do: Complete simulations with match into cooling
channel!
Optimizations
Scenario reoptimization
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Energy projection