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1 Dejan Trbojevic Muon acceleration by RLA with the non-scaling FFAG
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2 RLA for Muons Introduction: 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: Use the permanent magnets for the arcs – Halbach magnets. Try to make four or five times in muon energy by either a race track or dog- bone acceleration with a single arc (2.5-10 GeV or -60%< δp/p< +60%). 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 BNL - Muon Collider Design Workshop Dec 1-3, 2009
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3 ‘ Racetrack’ vs ‘Dogbone’ RLA (both + and - species ) E/2 EE better orbit separation at linac’s end ~ energy difference between consecutive passes (2 E) 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 From Alex Bogacz presentation at the previous LEMC: Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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4 1-pass, 3-5 GeV phase adv. drops much faster in the horizontal plane Triplet FODO vs Triplet focusing ‘flat focusing' linac profile* Bob Palmer* From Alex Bogacz presentation at the previous LEMC: 256.82 meters Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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5 The linac – Betatron Function dependence on energy Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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6 Multipass Linac - racetrack FFAG Chicane Non-scaling FFAG arc 20 Cavities Non-scaling FFAG arc Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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7 Muon Collider Review Meeting At BNL 2001
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8 Design of the arcs with Halbach magnets FODO cells for the 2.5 -> 10 GeV muons N=170 cells L=1.606 m L BD =0.73 m L QF =0.52 m For the: p/p=+-60% B BD =2.5 T GF=40.0 T/m GD=-50.0 T/m r=43.42 m 86.85 m Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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9 x max =65.8 mm x min = -35.1 mm 1.606 m 0.73/2 m 0.1675 m FODO cell for the p/p=+-60 % -> 2.5 - 10 GeV Arc cell with Halbach magnets 52 mm Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009 0.73/2 m
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10 x max =52.9 mm x min = -12.8 mm 1.606 m 0.73 m 0.1675 m FODO cell for the p/p=+-60 % -> 2.5 - 10 GeV Arc cell with Halbach magnets 52/2 mm Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009 0.52/2 m
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11 FODO cell for the p/p=+-60 % -> 2.5 - 10 GeV Arc cells for two different lattices Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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13 A total difference in the path length - 10 GeV and the minimum of the parabola is l=0.2465 m
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14 Halbach permanent magnet But in reality it would be limited by: (1)The realistic size (2)The demagnetization effect
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15 Permanent Magnet for the BNL additional triplets (K. Halbach) Y (cm) X (cm) Field Quality @ R=6 cm b2 = 10248.0 Gauss (17 T/m) b6 = 44.3 Gauss (4.3E-3) Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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16 Halbach permanent magnets: available material No-Fe-B Type Rare Earth Magnets:
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17 Halbach permanent magnets – pictures from the original publication: QL D = 52 cm BL = 16.75 cm QL F = 73 cm G F = 2.7 T/0.068 m = 40 T/m G D = -2.7 T/0.054 m=-50 T/m 14 cm 85 cm B g = B r ln(OD/ID) B r =1.5 T OD=85 cm ID =14 cm ln(OD/ID)=1.8 B g =2.7 T Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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18 Halbach permanent magnets 35 cm Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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19 The matching cell length is: L=3 * 1.605 m = 4.815 m Matching cell – geometrical constraint - arc to linac Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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20 IEEE Transactions on Nuclear Science, Vol. NS-30, No. 4, August 1983 Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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21 Yoshiharu Mori – Fermilab FFAG workshop:
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22 Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009 Yoshiharu Mori – Fermilab FFAG workshop:
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23 Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009 Yoshiharu Mori – Fermilab FFAG workshop:
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24 Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009 Yoshiharu Mori – Fermilab FFAG workshop:
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25 Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009 Shinji Machida – Fermilab FFAG workshop
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26 New matching cell ff ff dd lolo x max x min a max u min u max do dmin dmax fmin fmax fo dd dd dd a min Input parameters are: x max and x min from the arc NS-FFAG p max, p o, and p min, D x, x, y, Unknowns: B D, B F, fo, do, and l o To be matched to the input parameters of the linac: x, y, x, y Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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27 Matching Cell - @ zero dispersion end dd dmax dmin a max a min dmin dmax do u max u min lolo Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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28 Matching Cell @ entrance p min p max popo x max x min a max a min fmax fo fmin fmax fmin fo u max u min fmin - fo fo - fmax w j lolo u max =a max +l o tan( fo - fmax ) u min =a min +l o tan( fmin - fo ) fmax fo - fmax = do - dmax fmin - fo = dmin - do Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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29 Mike Craddock’s approach: ff ff dd lolo x fp+ x fp- X d+ u min u max do dmin dmax fmin fmax fo dd dd dd X d- low p - high p + popo F/2 D/2 x d+ =0 x d- =0 Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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30 Matching to linac -> zero dispersion for each momentum Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009 Orbit offsets Dispersion yy xx
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31 Matching to linac -> zero dispersion for each momentum 10 GeV 2.5 GeV Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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32 p>p cent orbits matched to linac -> zero dispersion for each momentum p=p cent p=p max Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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33 Matching cell to the non-scaling FFAG arcs Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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34 Matching cell to the non-scaling FFAG arcs Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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35 Non scaling FFA arcs with matching cells without linac Orbits from 2.5 – 10 GeV through the matching cells and arcs: Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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36 Non scaling FFA arcs with matching cells without linac Betatron Functions from 2.5 – 10 GeV through the matching cells and arcs: Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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37 Non scaling FFA arcs with matching cells without linac Dispersion from 2.5 – 10 GeV through the matching cells and arcs: Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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38 Matching cell with linac – arc to linac Orbits magnified 100 times From 2.5 GeV- 10GeV Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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39 Multipass Linac with combined function triplets Details of the orbits with Chicanes: Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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40 Details of the chicane calculations: LoLo L L o /L=cos Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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41 Details of the Chicane CAVIT Y TRIPLET Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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42 Summary: A combination of the non-scaling FFAG with linac is possible. Time of flight adjustments is necessary –maximum of 0.493 m delay. The simulation of acceleration can be set-up by the PTC (Polymorphic Tracking Code). Thanks to Muon Inc. for the support Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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43 Shinji Machida – Fermilab FFAG workshop
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44 Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009 Shinji Machida – Fermilab FFAG workshop
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45 Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009 Yoshiharu Mori – Fermilab FFAG workshop:
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46 Dejan Trbojevic BNL - Muon Collider Design Workshop Dec 1-3, 2009
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47 Yoshiharu Mori – Fermilab FFAG workshop:
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