1 Front End for MAP Neutrino Factory/Collider rf considerations David Neuffer May 29, 2014.

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Presentation transcript:

1 Front End for MAP Neutrino Factory/Collider rf considerations David Neuffer May 29, 2014

2Outline  Previous baseline was 200 MHz (IDS nu Factory)  Rf, power req.  Front End for MAP NF/MC 325 MHz  Bunch train shorter than IDS …  With Chicane/Absorber  Current baseline Use short taper  Variations under study

325MHz System “Collider” 325MHz System “Collider”  Drift  20T  2T  Buncher  P o =250MeV/c  P N =154 MeV/c; N=10  V rf : 0  15 MV/m (2/3 occupied)  f RF : 490  365MHz  Rotator  V rf : 20MV/m (2/3 occupied)  f RF : 364  326MHz  N=  P 0, P N  245 MeV/c  Cooler  245 MeV/c  325 MHz  25 MV/m  cm LiH absorbers /0.75m 3

325 Collider Update w / Chicane / Absorber 325 Collider Update w / Chicane / Absorber  Add 30 m drift after chicane * 6.5 m  +15°,-15º  Add chicane + absorber particle MeV/c particle MeV/c  absorber at 41m 10 cm Be particle MeV/c particle MeV/c  Bunch (N = 12) 0  15 MV/m: 496  365 MHz  Rotate (N= )– 20 MV/m: 365  MHz  Cool -325 MHz -25 MV/m P ref = 245 MeV/c p 6 m ~22m FE Targ et Solenoid Drift BuncherRotatorCooler ~21m 24 m ~80 m π  μ 15m drift +13m chicane m drift 0.1 m Be Chicane + Absorber SREGION ! bentsol e BSOL VAC NONE

ICOOL results  325 “muon collider” with chicane absorber  with added drifts between chicane and absorber ~30 m  ~ μ/p  but smaller emittance beams scraped to better fit?  Change to shorter taper  15 m  6 m  (Hisham) slight improvement in throughput (~ 5%)  We are using Hisham’s more recent distributions Gains ~ 5-10% Total is now ~ μ/p (in baseline ICOOL simulation units)  Better Rotator/Cooler match (Diktys)  +5%  Cooler will be replaced by better 6-D cooler (Alexahin) 5

Compare 325 w chicane vs old z=38m z=137m z=255m High P cutoff is ~700 MeV/c (from ~500 MeV/c) GeV/c

7 Rf cavity Concept designconstruction operation

8 MAP rf properties (~ MICE rf)  Assume pillbox, Cu walls  Compare with MICE rf  Q = ~58000  a=0.574m, L=0.5, f=200MHz  T t =0.83  P 0 = 1.35 MW at 10MV/m  f=200MHz, L=0.5m, E 0 =10MV/m  U 0 = 62J, T fill = 63.7μs  P 0 = 3MW at 15MV/m MICE rf parameters Value Radius (mm)610 Length (mm)430 RT 2 (M  /m)22 Power needed (16MV/m) 4MW Quality factor, Q 0 54,000

9 IDS RF requirements  Buncher  37 cavities (13 frequencies)  13 power supplies (~1—3MW)  RF Rotator  56 cavities (15 frequencies)  12 MV/m, 0.5m  ~2.5MW (peak power) per cavity  Cooling System – MHz  m cavities (75m cooler), 15MV/m  ~4MW /cavity Front End section Length#rf cavities frequencies# of freq. rf gradientrf peak power requirements Buncher33m to to 7.5~1 to 3.5 MW/freq. Rotator42m to ~2.5MW/cavity Cooler75m MHz115 MV/m~4MW/cavity Total drift)~240m19329~1000MV~550MW Magnet Requirements: rf

10 Rf Buncher/Rotator requirements  Buncher -21m  37 cavities (14 frequencies)  13 power supplies (~1—3MW)  RF Rotator -24m  64 cavities (16 frequencies)  20 MV/m, 0.25m  ~2 MW (peak power) per cavity  Cooling System – MHz  m cavities (75m cooler), 25MV/m  ~4MW /cavity Front End section Length#rf cavities frequencies# of freq. rf gradientrf peak power requirements Buncher21m37484 to to 160—1.34 MW/cavity Rotator24m56364to ~2.4 MW/cavity Cooler75m MV/m~3.7MW/cavity Total df+bxr+rttr ~134m9330~500MV140MW rf

First result on discretization 11

Dependence on rf gradient  With same cooling channel  25MV/m IDS 4-D cooling  Change Buncher/Rotator peak rf voltage  0 –25 MV/m  Longer bunch train captured with larger V’ 12 0 MV/m 10 MV/m 20 MV/m

Dependence on B final 13

Summary  We are studying 325 MHz based front end  produces more bunches in same length bunch train than 200 MHz  requires more bunches to be recombined ~12  21 more difficult … ? HCC recombiner ?  Including chicane/absorber Improved matching  Would like to fit more μ in fewer bunches 14

Current Status 15 P5 process: P5 Result:

Supplemental slides 16

325 (w chicane/absorber) GeV/c 0.0 GeV/c  ~60 m long bunch train  ~ MHz buckets  For collider choose “best 21 bunches “  (~19m)  Includes ~2/3 of captured μ’s  many are lost  21bunches are recombined to 1 in collider scenario  It is more difficult to recombine 21 than 12  Would like to extend acceptance or generate shorter train 0m 65m 93m 131m 215m ~ end of rotator ~ After ~80m

P5 result 18