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COMET Task Force
COMET Task Force Report
7th J-PARC PAC meetingSatoshi MIHARAIPNS, KEK
COMET Task Force
Task Force
MembersS.Mihara, N.Saito, K.Yoshimura (KEK)M.Ieiri, K.Tanaka (KEK, Beam line experts)T.Ogitsu (KEK, SC magnet expert)A.Ando, K.Oide, M.Tomizawa (KEK, Acc experts)M.Aoki, A.Sato (Osaka Uni.)
Goal (defined by ourselves)In order to realize an experiment that can provide significant physics
result, the task force aims at showing a realistic solution(s) for theexperiment under discussions among experts from accelerator, beamchannel, and physics groups.
If possible a task force should be set up to consider the specialdemands of the required beam structure, energy, and intensity.Reports from these committees should be made to the PAC inupcoming meetings…. Minutes of the 4th PAC meeting
COMET Task Force
Tasks• Proton beam acceleration
– Investigation of the method described in the proposal– Other possibilities to produce required proton beam structure
• Extinction– 10-9 level necessary to reach 10-16 sensitivity– Development of measurement technique
• Proton beam extraction/transport– Proton beam transport to the target– Radiation shield around the target– Beam dump
• Experimental space– Possible location(s)
• In the current experimental hall• Extension of the current hall
COMET Task Force
Outline
•Proton Beam Acceleration
•Extinction Study Status
•Proton Beam Extraction/Transport
•Experimental Space
COMET Task Force
Proton Beam Acceleration
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Proposed Method (I)• RCS: h=2 with one empty
bucket• MR:h=9 with 5 empty buckets• Bunched slow extraction
– Slow extraction with RF cavityON, 210kV
Realization of an empty bucket inRCS by using the chopper in Linac
•Simple solution
•No need of hardware modification
•Heavier heat load in the scraper
•Possible leakage of chopped beam inempty buckets
COMET Task Force
Proposed Method (II) & (III)
Space charge tune shift is half of (I)Longitudinal emittance is twice of (I)NO EMPTY BUCKET IN RCSRCS RF system needs minormodification (low level RF)
NO EMPTY BUCKET BOTH IN RCS ANDMRSpace charge tune shift is half of (1)LARGE MODIFICATION OF MR RFSYSTEM IS NECESSARYLong bunch
COMET Task Force
Proton Acceleration Prospect
•Try method (I) first for an extinctionstudy– No hardware modification is necessary– Investigate
•Time structure of the proton beam•(Heat load at chopper)•RF voltage while extraction
•Method (II) may be tested if h=1operation of RCS is realized for MRintensity upgrade– Check how extinction can be improved
COMET Task Force
MR Simulation• It will be useful to study the growth of beam
structure by a simplified simulation from theview point of “particle leakage from a bucket toanother”.
• FNAL Mike Syphers’s demonstration
•To simulate realsituation, we need tounderstand
•RF noise•Real shape(including the tail) ofthe beam in thephase space
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Extinction Study
Extinction Study
•Extinction measurement usingsecondary beam
•Extinction measurement using a newabort line monitor
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COMET Task Force
Measurement at K1.8BR• Measure secondary particle
time structure relative to areference signal from the MR– We need
• MR RF signal in theexperimental area
• Beam line hodoscope countersat the K1.8BR line
– Support by E15/E17 group• MR operation with empty
buckets• Bunched slow extraction
– Count the number ofsecondary particles as afunction of time
• Particle identification– TOF
• Integration for ~103 secondssupposing 1MHz counting rate
Delayed reference signals Counter signal
COMET Task Force
Abort Line Monitor• Utilize beam monitor in the abort line• Single bunch & single shot operation of the MR
– Look at the empty bucket before the filled one– Detector that can count the number of protons
• Two layers of hodoscopes– Plastic scintillator and quarts– Support by thin carbon fiber plates– Read by Multi-anode PMT through optical fibers– Operated in the beam line vacuum
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Detector is Ready to Install• Cosmic-ray test OK• Evacuation test OK• Outgassing rate 10-5m3Pa/s
– Turbo pump near thedetector
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Signal Quality Test• Need to transfer PMT signal
– from the abort line to thecounting room
– through 300m long cable• Very special cable
• Can we see PMT signal?– Tested using a normal
scintillation counter with PMTreadout
COMET Task Force
When beam is dumped…• Triggered by the abort line kicker excitation signal
– “Signal” seen ~20 µsec later and continued for 20µsec– Smaller pulses continued even after that for ~10msec
• No “signal” and No noise before that!
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During acceleration• 180msec later after the start of acceleration• Clear correlation between “signal” and RF reference signal• Measurement using PMT is feasible to study time structure of the
primary proton beam
RF reference signal
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Proton BeamExtraction/Transport
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Bunched Slow Extraction
8GeV energyh=9, RF cavity ON, 210kVEL=3eVs, matched ellipse
Before extraction at ESS Extracted beam at ESS
70nsec
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Effect of ESS foil• Example of simulation (done
for 50GeV study) usingMARS– 40cm downstream from ESS
exit
– “real loss”=N(hit p) –N(scattered p)/N=0.14%
– Remaining protons
– Scattered to extraction side
– Scattered to circulation side
• Need to redo the simulationfor J-PARC configuration
Scattered to extracted side
Scattered to circulating side
COMET Task Force
Beam optics calculation :TRANSPORT+G4Beamline
Proton Beam Transport
TRANSPORT
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AC Dipole Section
B=600GB=0G
AC dipole Field
- G4Beamline• TRANSPORT
- G4Beamline• TRANSPORT
Optics Layout
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Extinction Improvement•Extinction improvement >103
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Experimental Space
COMET Task Force
Experimental Space
• Radiation– Difficult to move the target and dump after the
experiments completes
• Interference with other experiments– Day-1 experiments at K1.1 and K1.1BR– Primary beam experiments using B-line
• Electricity and cooling water– Power supplies for magnets– Refrigerator for the capture solenoid
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A Possible Layout
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Another Possible Layout
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Power Supply and Refrigerator• At least two power supply units
of 5000-10000A 10V• 200W class He refrigerator
– cold box, dewar, compressor– He Buffer tank of 100m3
– LN2 storage• 80-100m2 for these
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Summary
• Extinction tests– Abort line monitor measurement
– Detector is ready to install– Single bunch & single shot operation of MR
– Secondary beam line (K1.8BR) measurement– method (I) (5 empty and 4 filled buckets) operation with
bunched slow extraction• Need more simulation work for better
understanding of– possible leakage of beam during acceleration– extraction
• Layout of the experiment– Feedback from the COMET group