opportunities for experiments based on stored muon beams at fermilab milorad popovic jean-francois...
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Opportunities for Experiments Based onStored Muon Beams at Fermilab
Milorad PopovicJean-Francois Ostiguy
FermilabAugust, 2014
Motivation• Measure neutrino cross-section with better than 10%
precision • Take advantage of the existing accelerator complex
configuration providing beam to the New Muon g-2 Experiment
• Utilize existing detectors (MicroBooNE, ICARUS)• Minimize initial investment. Providing a suitable building to
house the detector would be the only investment required • Describe possible improvements in collecting and storing
muons that would allow cross-section measurements with a precision of a few percent with a modest additional investment.
• Provide a suitable test facility for future NF
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The Context
• We revisit the idea of using the Debuncher as a storage ring for muons
• the g-2 Experiment expects 6x10-6 stored muons per 8 GeV proton on target
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g-2 Experiment• Booster pulse(5x1012 Protons@ 8 GeV) is separated in 4
bunches (~100 ns long) in the Recycler• The Booster is a 15 Hz machine (not all cycles are used)• Target Station is AP0 (Antiproton production target station)
and was run with beam power up to 72 kW ( 120 GeV beam from Main Injector)
• 3.1 GeV/c Pions/Muons are collected using Lithium Lens ( this lens was used for collection of 8.9 GeV/c Antiprotons with ~0.5 Hz)
• Debuncher is used as delay line for muons (beam is stored for 3 turns).
• Muons go to g-2 storage ring for experiment.
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Concept: g-2 Experiment 6x10-6 stored muons in the Debuncher per 8 GeV proton on target
Booster/Linac
Extraction from RR
Injection to RR
NEW TRANSFER LINE
A3 lineA2 line
Main Injector
F0P1 line
MI-52
MI-30
p
Recycler
_p
MI-10
Pbar
AP0
P2 line
Accelerator Overview
INJ8GeV
G4BeamLine simulations of g-2
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• In simulation 1.4x1010 protons on AP0 target
after Li lens
at end of transfer line
after one turn Debuncher
g-2 simulations
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6x10-6 stored muons in the Debuncher per one 8 GeV proton on target
after Li lens
at the endof transfer line
after one turn in Debuncher
Proton Beam Like for g-2,but with g-2 off
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• 5x1012 protons in a Booster pulse• 3 Hz, 8 GeV Booster• Muons are stored for ~100 turns• Running time 107 Sec (1 year)• 100 ton detector, 10 meters downstream from ring
~ 400 CC neutrino events
This is for about the cost of moving an existing detector (BooNE??, 60T) and building a new detector housing (about 3M$)
Looking in the near future ( cost~$0.0)
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• 1x1013 protons from MI (two Booster pulses slip stacked)• 1 Hz, 120 GeV MI• Muons are stored for ~100 turns• Running time 107 Sec• 100 ton detector, 10 meters downstream from ring
~ 5x400 CC neutrino events
Looking Into the Future ( cost~$??)
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• 1x1013 protons from MI (two Booster pulses, slip stacked)• 1 Hz, 120 GeV MI• New Li lens r = 2 cm to increase collection of pi’s ( x1.5) • Make ring to be racetrack (x 1.5)• Running time 107 Sec• Larger detector, ~500 ton detector( x5)
~ 1.5x1.5x5x5x400 CC neutrino events
G-2 simulations• Hi Milorad,
• Please find attached the momentum distributions of pions and muons at three different locations in the g-2 beamline:
• START - after the Li lens • VD5 - at injection into the Debuncher Ring• STOP - after one revolution around the Debuncher Ring.
• For normalization, the number of incident 8-GeV-energy protons in this simulations was 1.47e10.• The simulations were conducted using the so-called "default" parameters of the proton beam spot
size on the target (sigma_x=sigma_y=0.5 mm) and the Li-lens. With an additional optimization of the proton beam parameters (reducing the spot size on the pion production target) and optimization of the Li-lens position relative to the target at given field strength, the yield of the muons can be increased by may be additional ... 30%(?) -- I don't have a precise number for this.
• The "magic momentum" is 3.094 GeV/c.
• Hopefully this helps. If you have any questions, please don't hesitate to contact me.
• Best regards,• Volodya
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