Neutrino Town Meeting Neutrino Town Meeting CERN – May 14-16, 2012 CERN – May 14-16, 2012 SPL R&D and Potential SPL R&D and Potential Applications Applications R. Garoby for the SPL team* O. Brunner, S. Calatroni, O. Capatina, E. Ciapala, F. Gerigk, E. Montesinos, V. Parma, K.M. Schirm, + I. Aviles Santillana **, R. Bonomi **, J. Chambrillon, P. Coelho Azevedo**, K. Liao, N. Valverde Alonso** ** supported by ESS
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Neutrino Town Meeting CERN – May 14-16, 2012 SPL R&D and Potential Applications R. Garoby for the SPL team* O. Brunner, S. Calatroni, O. Capatina, E. Ciapala,
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Neutrino Town MeetingNeutrino Town MeetingCERN – May 14-16, 2012CERN – May 14-16, 2012
SPL R&D and Potential SPL R&D and Potential ApplicationsApplications
R. Garoby for the SPL team*
O. Brunner, S. Calatroni, O. Capatina, E. Ciapala, F. Gerigk, E. Montesinos,V. Parma, K.M. Schirm,+ I. Aviles Santillana **, R. Bonomi **, J. Chambrillon, P. Coelho Azevedo**, K. Liao, N. Valverde Alonso**
** supported by ESS
HP-SPL:HP-SPL:R&D ManagementR&D Management
R. G. – 15/05/2012 3
• R & D for a High Power SPL formally supported at CERN in view of multiple future potential applications
~1.7 MCHF and 6 FTEs / year
• Collaboration with ESS Fellows and procurement of klystron modulator for SM18
• French in-kind contribution Tuners, Helium tanks, use of Saclay 704 MHz high power test place…
• EC-supported programmes• EuCARD (WP10)
Development and test of beta=1 (CEA) and beta=0.65 (IN2P3) 5 cells cavities• CRISP (WP4)
Joint work with ESS and DESY EC-supported manpower for upgrading and exploiting the SM18 test place
• LAGUNA-LBNO EC-supported fellow for studying proton drivers at CERN using LP- or HP-SPL
• DOE-supported programme• BNL Development and test of a =1 cavity
ResourcesResources
SPL documentation in EDMS [ https://edms.cern.ch/nav/SLHC-000008 ] SPL meetings in Indico [ http://indico.cern.ch/categoryDisplay.py?categId=1893 ]
SPL documentation in EDMS [ https://edms.cern.ch/nav/SLHC-000008 ] SPL meetings in Indico [ http://indico.cern.ch/categoryDisplay.py?categId=1893 ]
«Project-like» structure aimed at meeting the objectives of the HP-SPL R&D:• Building and testing a prototype cryomodule with 4 cavities• Updating CERN infrastructure and competence in superconducting RF technology• Preparing submission of future subjects of R&D [design and construction of a full-size cryomodule,
high power RF sources, HIPIMS (High Power Impulse Magnetron Sputtering)…]
Work UnitsWork Units-Design, construction and test of the prototype cryomodule (Leader: V. Parma)
- Components: Cryomodule, Cavities, RF items (Couplers, tuners, …), cryogenics equipment…- Assembly (with adequate tools): cavities string in clean room, inclusion in cryomodule- Tests: cavities in vertical cryostat, assembled cryomodule in bunker.- Upgrade of the SM18 infrastructure (Leader: O. Brunner)- HP water rinsing system and upgraded clean roon- Cryogenics for efficient operation at 2K- High power RF at 704 MHz (klystron, modulator, high power distribution)- Low Level RF and controls
-SC RF cavities technology (Leader: E. Ciapala)- Fabrication and processing- Test, diagnostics and analysis
Energy range: 160 MeV – 732 MeV5 cell cavitiesGeometrical : 0.65Maximum energy gain: 19.4 MeV/m54 cavities (9 cryomodules)Length of medium section: ~110.35 m
Energy range: 732 MeV – 5 GeV5 cell cavitiesGeometrical : 1Maximum energy gain: 25 MeV/m192 cavities (24 cryomodules)Length of high section: ~360 m
Short cryomodule: vacuum vesselShort cryomodule: vacuum vessel
R. G. – 15/05/2012 22
4.5 K vapor generatorreservoir (with elect.heater)
standard support
Last cavity IC support
Ph.Separator pot
DN80 gate valve (single valve)
CWT 50 K heat intercept
(views S.Rousselot, IPN-Orsay)
Short cryomodule: technical service Short cryomodule: technical service modulemodule
Courtesy P.Duthil (IPNO)
R. G. – 15/05/2012 23
Courtesy W. Hofle @ 5th SPL collaboration Meeting
D. Valuch
LLRF under developmentLLRF under development
R. G. – 15/05/2012 24
Upgraded installation in SM18Upgraded installation in SM18
R. G. – 15/05/2012 25
Delivery of 704 MHz klystron and modulator
Preparation of SM18 infrastructure (cryogenics, RF, clean-room)
Cavities production
Cavities processing/RF testing
RF couplers
Clean room assembly of string
Cryomodule (& assy tooling) design
Cryomodule fabrication
Cryomodule assembly
Start cryomodule RF testing
Short cryomodule: master scheduleShort cryomodule: master schedule
R. G. – 15/05/2012 26
Related R & DRelated R & D
Nb coating of Cu cavities, using the HIPIMS (High Power Nb coating of Cu cavities, using the HIPIMS (High Power Impulse Magnetron Sputtering) technologyImpulse Magnetron Sputtering) technology
– In collaboration with Sheffield Hallam University (UK).– Supported in the context of the construction of LHC spare cavities.– Potentially very attractive technology for the SPL (raw material cost, mechanical Potentially very attractive technology for the SPL (raw material cost, mechanical
stiffness).stiffness).– First results on low beta 704 MHz cavity: end 2012First results on low beta 704 MHz cavity: end 2012
Max. bunch intensity LHC (25ns) ppb 4.0 x 1011 1.7 x 1011
Max. pulse intensity LHC (25ns) ppp 6.7 x 1013 1.2 x 1013
Max. pulse intensity FT ppp 1.0 x 1014 3.3 x 1013
Linear ramp rate T/s 1.5 2.2
Repetition time (50 GeV) s ~ 2.5 1.2/2.4
Max. stored energy kJ 800 70
Max. effective beam power kW 320 60
29
R. G. – 15/05/2012 30
PS2 integration at CERN: reminderPS2 integration at CERN: reminder
30PAC 2009 Vancouver PS2 Design Optimization, M.Benedikt
PS2
SPL
Linac4
SPL to PS2
PS
PS/LEIR to SPS / PS2
SPS
PS2 to SPS
– “Straight” H- inj. line SPL PS2 avoiding large bending radii to minimise Lorentz stripping of H-.
– Minimum length of inj. line TT10 PS2 for ions and protons from PS complex.
– Minimum length HE line PS2 SPS.
R. G. – 15/05/2012 31
SPL-based 5 GeV – 4 MW proton drivers have been designed [SPL + 2 fixed energy rings (accumulator & compressor)] which meet these requirements
References:– SPL based proton driver/ R. Garoby, talk at NuFact06,
http://nufact06.physics.uci.edu/Workshop/Slides/RGaroby_SPL3_Pdriver.ppt– Feasibility Study of Accumulator and Compressor for the 6-bunches SPL-based Proton Driver / M. Aiba,
CERN-AB-2008-060– A first analysis of 3-bunches and 1-bunch scenario for the SPL-based Proton Driver / M. Aiba, CERN-AB-
Note-2008-048-BI– Beam Stability in the SPL Proton Driver Accumulator for a Neutrino Factory at CERN / E. Benedetto,
http://nufact09.iit.edu/wg3/wg3_benedetto-splstability.ppt, to be published– SPL-based Proton Driver for a Neutrino Factory at CERN, M. Aiba, E. Benedetto, R. Garoby, M. Meddahi,
poster nb.25 (this workshop)
Parameter Basic value Range
Beam energy [GeV] 10 5 - 15
Burst repetition rate [Hz] 50 ?
Number of bunches per burst (n) 4 1 – 6 ?
Total duration of the burst [s] ~ 50 40 - 60
Time interval between bunches [s] (tint)
16 ~ 50/(n-1)
Bunch length [ns] 2 1 - 3
Specifications(from ISS report)
HP-SPL based proton driver: principle HP-SPL based proton driver: principle (1/2)(1/2)
» Charge exchange injection» n x 100s accumulation time» Isochronous (=0): beam frozen longitudinally to preserve p/p » No RF (=> minimum impedance)» 1-6 bunches of ~120 ns length
2. Bunch compression- Compressor ring
» Large RF voltage (large stored energy & minimum RF power) (=> bunch rotation on stored energy)
» Large slippage factor => rapid phase rotation in few x10s, » ~2ns rms bunch length @ extraction to the target (=> moderate Q
because of dispersion)
• Synchronization between rings- Ratio of circumferences guaranteeing correct positioning of successive bunches inside the compressor without energy change in any ring
HP-SPL based proton driver: principle HP-SPL based proton driver: principle (2/2)(2/2)
R. G. – 15/05/2012 33
Accumulation Duration = 400 s
Compression t = 0 s
t = 12 s
t = 24 s
t = 36 s
etc. until t = 96 s
Accumulator[120 ns pulses
-60 ns gaps]
SPL beam[42 bunches -
21 gaps]Compressor
[120 ns bunch -V(h=3) = 4 MV]
Target[2 ns bunches
– 6 times]
Generation of 6 bunchesGeneration of 6 bunches
R. G. – 15/05/2012 34
-40 -20 0 20 40-2
-1
0
1
2
x' (
mra
d)
x (mm)
Injection Rotated
-10 -5 0 5 10-0.6
-0.4
-0.2
0.0
0.2
0.4
0.6 Injection Rotated
y' (
mra
d)
y (mm)
-40 -20 0 20 40-0.15
-0.10
-0.05
0.00
0.05
0.10
0.15 Injection Rotated
dE (
GeV
)
RF phase/3 (deg.)
-3 -2 -1 0 1 2 30
5
10
15
Cou
nts/
bin
(%, b
in=
0.2
deg)
RF phase/3 (deg)
Rotated=1.98 ns
from M. Aiba
Bunch rotation before ejectionBunch rotation before ejection
R. G. – 15/05/2012 35
SPL for proton driver Output beam Parameters Values Parameters Values
Kinetic beam energy 5 GeV Kinetic beam energy 5 GeV Repetition rate 50 Hz Repetition rate 50 Hz Average current during the burst 40 mA No. of bunches per cycle 6 Beam power 4 MW Bunch length (r.m.s.) ~2 ns Bunch spacing ~12 s
Circumference 318.5 m Circumference 314.2 m Transition gamma 6.33 Transition gamma 2.3 RF voltage - RF voltage 4 MV Harmonics number - Harmonic number 3 No. of arc cells 24 No. of arc cells 6 Super periodicity 2 Super periodicity 2 Nominal transverse tune 7.77/ 7.67 Nominal transverse tune 10.79/5.77 No. of turns for accum. 400 No. of turns for comp. 36 Maximum no. of bunches 6 Maximum no. of bunches 3
Main quadrupole Bore radius Field gradient Magnetic length
56 mm 5.5 T/m 1.2 m
Main quadrupole Bore radius Field gradient Magnetic length
148 mm 7.1 T/m 1.9 m
Main bending Full gap Full width Field stength Magnetic length
103 mm 162 mm
1.7 T 1.5 m
Main bending Full gap Full width Field strength Magnetic length
125 mm 379 mm
5.1 T 3 m
from M. Aiba
Main parametersMain parameters
R. G. – 15/05/2012 36
K1
K2
D1
D2
D3
D4
T1
T2
T3
T4
p z
Beam delivery on 4 targets & hornsBeam delivery on 4 targets & horns
Principle:• Use of 2 bipolar kickers (or bipolar pulsed magnets): ± 45˚ rotation wrt the z axis• K1 (K2) deflects to D1 and D3 (D2 and D4)• Need of 1 compensating dipole per beam line (1 angle for each target):
Apply a symmetry in the system
keff
EL
B
2998.0
)sin(Angle of deflection (rad)
Kinetic energy(GeV)Magnetic length (m)
Magnetic field (T)2000mm
T1 T2
T4 T3
z
K1 K2
D1 D2
D3 D4
T1 T2
T3 T4
zp
3D view
side view
E. Bouquerel – IPHC, EUROnu meeting, March 27, 2012
>>KEY PARAMETER<<
SummarySummary
R. G. – 15/05/2012 38
Technology (1/2)Technology (1/2)
Presently, the HP-SPL R&D:Presently, the HP-SPL R&D:
•progresses at a good pace, leading to the high power test of a short 4 cavities cryomodule in 2014.•allows testing the validity of new concepts that should result in significant savings (RF couplers, SS He tanks, Cryomodule design…)•can potentially be used in multiple projects at CERN as well as outside (ESS, MYRRHA) and benefits from external support (ESS and EU programmes)•is a means for CERN to embed inside the network of labs involved in superconducting RF technology (CEA, IN2P3, DESY, JLAB, FNAL, ANL…) and re-establish in-house competence in that field at the state-of-the-art level•drives infrastructural upgrades (e.g. electro-polishing facility, clean room, high power RF at 704 MHz…) which will be beneficial for other development (LHC main RF, Crab cavities, HIE IDOLDE…)
R. G. – 15/05/2012 39
Technology (2/2)Technology (2/2)
Important future R&D subjectsImportant future R&D subjects
•HOM damper for beam stability at high current•Cavities in view of reaching the expected performance/simplifying fabrication/evaluating alternative solutions (Nb on Cu)•Cryomodule towards a full size prototype•RF amplifiers for reducing cost•Power supply for high power amplifier for reducing cost
R. G. – 15/05/2012 40
Accelerator designAccelerator design
• The SPL accelerator design is «mature» and stable
• In the context of the LAGUNA-LBNO:– The LP-SPL design will be adapted to the requirements of the HP-PS– The HP-SPL design will be briefly revisited and completed with the design of the
accumulation ring
• Other applications may require resuming/refining accelerator design:– e+/e- acceleration in the ERL of the Linac-Ring option of LHeC– LEP-3– LP-SPL remains a back-up option for the LHC injector complex…