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Muon acceleration by RLA using non-scaling FFAG

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Presentation on theme: "Muon acceleration by RLA using non-scaling FFAG"— Presentation transcript:

1 Muon acceleration by RLA using non-scaling FFAG
Dejan Trbojevic Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

2 RLA for Muons Introduction: Problems: Goals:
Present design of the muon RLA’s Problems: Matching of the circular non-scaling FFAG to the straight linac. Time of flight adjustments for each pass. Goals: Try to make four or five times in muon energy by either a race track or dog-bone acceleration with a single arc ( GeV or GeV). Match the betatron and dispersion functions from the arc to the linac. Design a chicane to adjust the time of flight for different energy passes. Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

3 Few references for Mike Craddock:
D. Trbojevic E.D. Courant, and A. Garren, September 30, 1999, Montauk, Long Island High Energy Muon Collider Workshop Lee Teng: 1956 Non-scaling FFAG proposal at the conference A year later a book Conference Proceedings came out: D. Trbojevic, E.D. Courant, and A. Garren, “FFAG lattice without opposite bends” , AIP Conf. Proc. August 17, Volume 530, pp Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

4 ‘Racetrack’ vs ‘Dogbone’ RLA (both m+ and m- species )
From Alex Bogacz presentation at the previous LEMC: m- m+ m- m+ m- DE m+ better orbit separation at linac’s end ~ energy difference between consecutive passes (2DE) allows both charges to traverse the Linac in the same direction (more uniform focusing profile the droplets can be reduced in size according to the required energy both charge signs can be made to follow a Figure-8 path (suppression of depolarization effects) Chuck Ankenbrandt DE/2 m+ m- m+ m- Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

5 FODO vs Triplet focusing - ‘flat focusing' linac profile*
Bob Palmer* From Alex Bogacz presentation at the previous LEMC: Triplet 1-pass, 3-5 GeV meters phase adv. drops much faster in the horizontal plane Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

6 Design of the arcs – from the densely populated FODO cells for the 2
Design of the arcs – from the densely populated FODO cells for the 2.5 -> 10 GeV muons N=142 cells L=1.9 m LBD=0.9 m LQF=0.6 m For the: dp/p=+-60% BBD=1.64 T BQF =-1.09 T GF=20.8 T/m GD=-10.2 T/m r=42.94 m 85.9 m Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

7 Arc cells for two different lattices
FODO cell for the dp/p=+-60 % -> GeV x max=69 mm x min= -34 mm 1.9 m 0.3 m 0.9 m Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

8 Arc cells for two different lattices
FODO cell for the dp/p=+-60 % -> GeV Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

9 Matching cell – geometrical constraint - arc to linac
The matching cell length is: L=3 * 1.9 m = 5.7 m Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

10 Matching cell to the non-scaling FFAG arcs
Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

11 Non scaling FFA arcs with matching cells without linac
Orbits from 2.5 – 10 GeV through the matching cells and arcs: Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

12 Non scaling FFA arcs with matching cells without linac
Betatron Functions from 2.5 – 10 GeV through the matching cells and arcs: Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

13 Non scaling FFA arcs with matching cells without linac
Dispersion from 2.5 – 10 GeV through the matching cells and arcs: Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

14 The linac – Betatron Function dependence on energy
Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

15 Matching cell with linac – arc to linac
Orbits magnified 100 times From 2.5 GeV- 10GeV Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

16 Multipass Linac - racetrack FFAG
Chicane 20 Cavities Chicane Non-scaling FFAG arc Non-scaling FFAG arc Chicane 20 Cavities Chicane Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

17 20 cells linac Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

18 Multipass Linac with combined function triplets
Details of the orbits with Chicanes: Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

19 Path length difference from the arc cell dp/p=(0,-80%)
Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

20 Path length difference from the arc cell
(Ds=0.55m for arc) Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

21 Details of the chicane calculations:
Lo q -2q L Lo /L=cos q Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

22 Details of the Chicane CAVITY TRIPLET
Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

23 New approach: What do we need to came from a remainder by Yoshimaru Mori yesterday: IEEE Transactions on Nuclear Science, Vol. NS-30, No. 4, August 1983 Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

24 New matching cell Input parameters are:
xmax and xmin from the arc NS-FFAG pmax, po, and pmin, Dx, bx, by, Unknowns: BD , BF , Ffo , Fdo , and lo rfmax ffo rfo amax fdo amin rfmin ffo lo fdo umax xmax rdmin umin fdo xmin rdo fdo rdmax To be matched to the input parameters of the linac: bx, by, ax,ay Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

25 Matching Cell - @ zero dispersion end
amax amin lo rdmin umax fdmin rdo umin fdo rdmax fdmax Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

26 Matching Cell @ entrance
w Ffmax rfmax j rfmax Ffo amax rfo Ffo- Ffmax amin Ffmin Ffo- Ffmax= Fdo- Fdmax lo rfmin Ffmin- Ffo Ffmin- Ffo= Fdmin- Fdo umax pmin xmax umin umax=amax+lo tan(Ffo-Ffmax) po xmin umin=amin+lo tan(Ffmin-Ffo) pmax Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

27 Mike Craddock’s approach:
rfmax ffo xd+=0 rfo Xd+ fdo xd-=0 Xd- rfmin ffo lo fdo umax xfp+ rdmin high p+ umin fdo xfp- rdo po fdo low p- F/2 rdmax Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

28 p>pcent orbits matched to linac -> zero dispersion for each momentum
p=pmax p=pcent Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

29 orbits almost matched to linac -> zero dispersion for each momentum
10 GeV 2.5 GeV Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008

30 Thanks to Muon Inc. for the support
Conclusions: It looks like a combination of the non-scaling FFAG with linac is possible this could reduce present number of arcs. Multiple pass linac by the triplet combined function dipoles cells. Time of flight adjustments is necessary due to 0.6 m delay for the lowest energy pass through the arc. A details of chicane design has to be studied. Initial matching between the two arcs and linac could be improved. The simulation of acceleration with many particles is already set-up by the PTC (Polymorphic Tracking Code). Thanks to Muon Inc. for the support Dejan Trbojevic FFAG’08 Workshop, Manchester, 15:00, September 2, 2008


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