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A 10 GeV, 4 MW, FFAG, Proton Driver at 50 Hz G H Rees, RAL.

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Presentation on theme: "A 10 GeV, 4 MW, FFAG, Proton Driver at 50 Hz G H Rees, RAL."— Presentation transcript:

1 A 10 GeV, 4 MW, FFAG, Proton Driver at 50 Hz G H Rees, RAL

2 Non-scaling, Non-linear FFAGs Categories for FFAG Lattice Cells of Five Magnets: 1. IFFAG: isochronous, no Q v =n and 2Q v =n crossing 2. IFFAGI: IFFAG with combined function insertions 3. NFFAG: non-isochronous, high/imag  -t, no Q var’n 4. NFFAGI: NFFAG with insertions, some Q h variation 1 and 2: rapid acceleration of muons or electrons 3 and 4 : high power proton drivers or medical rings

3 4 MW Proton Driver Arrangement Muon yields optimal for GeV (S Brooks, RAL) Choose: 10 GeV, 50 Hz to reduce target shock 3 GeV booster for 3 – 10 GeV NFFAGI 2, 25 Hz or 1, 25 Hz booster (R =2.2 R b ) 0.18 GeV H ‾ linac for low bunch areas 5 bunches at h = 5 for RCS booster(s) Transfer: 5 (10 13 protons/bunch) to the NFFAGI Bunch to: 1 ns (rms) adiabatically (h = 33 & 198)

4 Longitudinal bunch area The longitudinal bunch area (in eV sec) is: A = (8Rα/(ch)) ((2 V(I-  sc )E o  ) / (h  )) ½ For a small longitudinal bunch area, choose a low value of injection energy and ring radius Choose E o (  - 1) = 0.18 GeV and R b  50.0 m Choose the bunch & harmonic number (h) = 5 Compressed bunch area needed  0.66 eV sec

5 4 MW, Proton Driver Layout 0.18 GeV H ‾ Achromat 0.18 GeV H ‾ Linac 10 GeV, 50 Hz, N = 5, NFFAGI with protons per bunch 3 GeV, 50 Hz, h =5, RCS (1 at 50 Hz, or 2 at 25 Hz)

6 NFFAGI Design Criteria For compression of the 5 bunches at 10 GeV: Design for a gamma-t value at 10 GeV  20 Design for longitudinal bunch areas  0.66 eV s Adiabatic acceleration & comp. with h = 33, 198 Design the NFFAG ring with lattice insertions, to ease injection, ejection & beam loss collection Use two insertions to allow most flexibility, eg: 21 normal and 13 insertion cells per insertion

7 Acceleration and Compression Systems Driver-booster circumference ratio: 2.2 to 1 Booster rf range (h=5): to MHz Driver rf range (h=33): to MHz Compression frequency (h=198): MHz Peak accelerating voltage per turn: 1.0 MV Peak compression voltage per turn: 2.56 MV

8 Lattice Cell Options Normal cell Insertion cell Magnet types Doublet D D1 + T0 + D Triplet T T1 + T2 + T Pumplet P1 P Easiest solution is to match P1 and P2 pumplet cells:  P1 has a smaller β-range than either D or T  The insertion has only one type of cell, P2  P2 has the smallest closed orbit “lever arm” No 2  dispersion suppressors, as too many are needed

9 10 GeV, Normal & Insertion Cell Layouts bd(-) BF(±) BD (+) BF(±) bd(-) O O Normal cell (5.294º, m) Insertion cell (5.294º, m) 2.2 There are two superperiods of 21 normal & 13 insertion cells At 10 GeV: Q v = 13.72, Q h = 19.36,  -t = 20.4, R = m

10 NFFAGI Lattice Design Use equal bend, normal and insertion, pumplet cells Arrange ~ matching for a normal and insertion cell Arrange integer, insertion tunes eg Q h = 4 & Q v = 3 The normal cells in an insertion are then matched Seek unchanged closed orbits on adding insertions by varying the normal cell field gradients and tunes Then, dispersion match is almost exact for insertions Small ripple remains in β h and β v (max) in insertions

11 Non-Linearity Compensation Crossing of the 3rd order resonance: 3Q h = 58  Insertion and arc 3(Q h ) values: 3Q h = 3(4, 5⅔ )  Hence, no 3rd order excitation for: 3Q h = 58 Crossing of 4th order resonance: 2Q h + 2Q v = 66  Insertion and arc values for: 2(Q h + Q v ) = 2(7, 9½ )  So, no 4th order excitation for: 2Q h + 2Q v = 66 Crossing of the 4th order resonance: 4Q h = 77  Insertion and arc 4(Q h ) values: 4Q h = 4(4, 5⅝ )  Some small 4th order excitation for: 4Q h = 77

12 NFFAGI Lattice Results Satisfactory matching at the 24 reference energies: 10.0…..6.8, 6.5…..5.0, 4.75…..4.0, 3.8…..3.0 GeV. Q v =13.72 throughout the 3 to 10 GeV energy range. Dispersion match is found by varying K(bd) and  h : T =10.0……6.8, 6.5…. 5.0, , 3.8…3.0 GeV Q h =19.36, 19.31, 19.3, 19.29, 19.2, 19.2, 19.2, 19.2 Gamma-t becomes imaginary for the low energies

13 Combined Function Magnet Fields (T) Magnets Insertion Normal cell bd to to BF 1.75 to to BD 0.54 to to 1.59 T max bending ratios; bd : BF : BD ~ : 1.0 : 0.23 (Ratios in muon ring; bd : BF : BD ~ : 1.0 : 1.0)

14 Beam Loss Collimators Vertical:  Locate in 4, adjacent, long, insertion straights  Use 1, primary and 3, secondary, 5 kW collimators  Use tapered units for lower, high energy acceptance Horizontal:  Locate in the first three, vertical, collimator straights  Use 1, primary and 3, secondary, 5 kW collimators  Use angled units for collimation at 3 and 10 GeV

15 10 GeV NFFAGI versus RCS Pros: Allows acceleration over more of the cycle, No need for ac magnet p/s or ceramic chamber, Gives more flexibility for the holding of bunches, Required is one NFFAGI ring, but two RCS(s), Allows operation at 50 Hz instead of at 25 Hz, with ppp at target, instead of ppp. Thus, there is half the target shock per pulse. Cons: needs a larger (~ 0.33 m) radial aperture


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