Title: NonScaling FFAG Accelerators for the Neutrino Factory Proton Driver
1Non-Scaling FFAG Acceleratorsfor the Neutrino
FactoryProton Driver
- Alessandro G. Ruggiero
- Brookhaven National Laboratory
- NuFact06 - Irvine University, California -
August 24-30, 2006
2Requirements
- Kinetic Energy 5 - 15 GeV 11.6 GeV
- Average Power 4 MW 4 MW
- Repetition Rate 50 Hz 50 Hz
- Number of Bunches 3 - 5 5
- Bunch Length (rms) 1 - 3 ns 2 ns
- Number of Protons 4.31 x 1013 per pulse
- Protons per Bunch 0.862 x 1013
3Architectures
- Rapid-Cycling Synchrotrons
- Super-Conducting Linacs
- FFAG (cyclotrons, RLA, microtrons, )
-
- SCL CEBAF
-
- Dog-Bone
- FFAG
- The case for a Non-Scaling FFAG
- A.G. Ruggiero, BNL Report C-A/AP/219, Oct. 2005
- also in proceedings of NuFact06, Frascati, June
2005
4FFAG Accelerators for Proton Driver
The scheme allows flexibility of choice of
energy, intensity, rep rate. It can suit any
requirements for muon production and collection
FFAGs are Non-Scaling of about the same
circumference and similar structure, located in
the same enclosure. Bunch Compression is done in
the last ring at the end of acceleration.
5Three - FFAG Accelerator Rings (1)
A.G. Ruggiero, 1.5-GeV FFAG Proton Accelerator
for the AGS Upgrade, Invited Talk to
EPAC-04, July 6-11, 2004, Lucerne, Switzerland.
6Three - FFAG Accelerator Rings (2)
7Three - FFAG Accelerator Rings (3)
Injection Injection
8 RF Frequency Power
MHz
MW
Injector Ring Low-Energy Ring High-Energy Ri
ng
turns
turns
MHz
MW
turns
turns
MW
MHz
turns
turns
9 Injector Ring and Injection
RF Ion Source ?
10Lattice Parameters
Non-Scaling Lattice
11 Lattice Functions
All Rings Linear Field Profile
Injection Extraction
12Tune Variation Radial Compactnesssame result
for all Rings
Half a Period
? (p - pinj) / pinj
13 Linear Field Distribution (kG vs. cm)
Injector Ring High-Energy Ring
Low-Energy Ring
14Extraction and Targetting
- The Revolution Period at Extraction from the
High-Energy Ring is T0 2.70 µs - Beam Bunches are extracted individually every n
turns -
- Pulse Duration
- n 1 n T0 2.70 µs 10.80 µs
- 2 5.40 21.60
- 3 8.10 32.40
- 4 10.80 43.20
- 5 13.50 54.00
15 Conclusions
- FFAG Accelerators for Neutrino Factories are
feasible - Issues
- Space Charge at Injection
- Multiple Resonance Crossing
- Injector Linac (400-MeV DTL or ????)
- Multi-turn Injection of H
- Magnet Feasibility
- Fast RF sweep (ferrite, RF power)
- Collimation
- Numerical Tracking
- Cost Estimate
- It is possible to raise the Repetition Rate --gt 1
kHz - or CW Mode of Operation (Harmonic Number
Jump)