NuFact 03 WG1 Summary€¦ · WG1 Summary NuFact03 , June 11, 2003 2 NuFact 03 WG1 Summary Future...
Transcript of NuFact 03 WG1 Summary€¦ · WG1 Summary NuFact03 , June 11, 2003 2 NuFact 03 WG1 Summary Future...
WG1 SummaryNuFact03 , June 11, 2003
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NuFact 03 WG1 Summary
Future ExperimentsG. Feldman Progress report from NUMI off-axis
R. Bernstein Independent study of NUMI off-axis sensitivity
K. Kodama Progress report on CNGS and Opera/Icarus
Y. Obayashi JHF progress report and θ13 sensitivity
J. Burguet- JHF intermediate detector
Castell
S. Kahn BNL/Homestake proposal
G. Rajasekaran A large iron detector for the neutrino factory
Y. Efremenko A long-baseline experiment in the IHEP tunnel
WG1 SummaryNuFact03 , June 11, 2003
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NuFact 03 WG1 Summary
Future ExperimentsLBL; approved, ongoing
K. Kodama Progress report on CNGS and Opera(/Icarus)
LBL; proposed, realistically studied
Y. Obayashi JHF progress report and θ13 sensitivity
J. Burguet- JHF intermediate detector
Castell
G. Feldman Progress report from NUMI off-axis
R. Bernstein Independent study of NUMI off-axis sensitivity
VLBL; conventional beam
S. Kahn BNL/Homestake proposal
Y. Efremenko A long-baseline experiment in the IHEP tunnel
VLBL; neutrino factory
G. Rajasekaran A large iron detector for the neutrino factory
WG1 SummaryNuFact03 , June 11, 2003
•CNGS: First beam to Gran Sasso: May, 2006
•OPERAEmulsion delivery to Gran Sasso starts
in August 2003Run from Day 1Emulsion analysis for event location
must be ready before Day 1Rehearsal for event location using
“mini-OPERA” at KEK-PS in 2004
•ICARUS (A. Rubbia, plenary talk)T600 installation at CNGS has been
approved in March 2003.Transported and installed in 2003-2004. T3000 = T600 + T1200 + T1200
WG1 SummaryNuFact03 , June 11, 2003
JHF-Kamioka Neutrino Experiment
~1GeV νννν beamKamiokaJ-PARC(Tokai)
0.75MW 50 GeV PS
( conventional νννν beam)
Super-K: 22.5 kt
Plan to start in 2007
Hyper-K: 1000 kt
4 MW 50 GeV PS
Y. Obayashi
WG1 SummaryNuFact03 , June 11, 2003
Neutrino BeamlineTransport line(Super-cond. Mag.)
Target station
Decay volume130m
Off-axis
Design in progress.
Budget request submitted.
Will be ready to start construction in 2004.
WG1 SummaryNuFact03 , June 11, 2003
Jun. 9, 2003 Y. OBAYASHI @ NuFact 03, Columbia Univ., New York 13
Detectors
Muon monitors @ ~140mFast (spill-by-spill) monitoring of beam direction/intensity
First Near detector @280mNeutrino intensity/spectrum/direction
Second Near Detector @ ~2kmAlmost same Eνννν spectrum as for SKWater Cherenkov can work
Realistic sensitivity studies and detector design studies started.
0
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x 10 3
0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5
Eν (GeV)
1.5km
295km
0.28km
Neutrino spectra at diff. dist
dominant syst. in K2K
p ππππ νννν
140m0m 280m 2 km 295 km
Role of the 2 km intermediate detector studied by Burguet-Castell: It will drastically simplify the systematic error analysis.
WG1 SummaryNuFact03 , June 11, 2003
There are some other longer baseline sites up to ~~~~950 km.
NuMI off-axisG. Feldman
WG1 SummaryNuFact03 , June 11, 2003
Active elements: scintillators or RPCs considered
Absorber: consensus to use particle board
WG1 SummaryNuFact03 , June 11, 2003
NuMI off-axis•LOI submitted August 2002 (P929)•Intention to submit proposal to November 2003 PAC•50 kton, 5 yr, 4××××1020 pot/yr
WG1 SummaryNuFact03 , June 11, 2003
R. Bernstein•Simulation studies of NuMI off-axis
•For ννννe appearance, simulated LAr and Fe/Scint, 100 kt/yr.
•Can see effects down to sin22θθθθ=0.01.
•LAr much better
WG1 SummaryNuFact03 , June 11, 2003
BNL →→→→ Homestake Super Neutrino Beam
2540 km
Homestake BNL
28 GeV protons, 1 MW beam power500 kT Water Cherenkov detector5×107 sec of running, Conventional Horn based beam
S. Kahn
WG1 SummaryNuFact03 , June 11, 2003
ννννe Appearance Measurements• a direct measurement of the
appearance of ννννµµµµ→→→→ννννe is important;the VLB method competes well withany proposed super beam concept
• for values > 0.01, a measurementof sin22θθθθ13 can be made (thecurrent experimental limit is 0.12)
• for most of the possible range ofsin22θθθθ13, a good measurement of θθθθ13 and the CP-violation parameterδδδδCP can be made by the VLB experimental method
νe APPEARANCE
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Reconstructed ν Energy (GeV)
Eve
nts
/bin
BNL-HS 2540 kmsin22θij (12,23,13) = 0.86/1.0/0.04∆mij
2 (21,32) = 7.3e-5/2.5e-3 eV2
1 MW, 0.5 MT, 5e7 sec
CP 135o: 591 evts
CP 45o: 449 evts
CP -45o: 300 evts
Tot Backg.: 146 evts
νe Backg.: 70 evts
DISCUSSION•1-ring QE event selection above a few GeV suffers from more BG.•More realistic BG estimation suggested.
WG1 SummaryNuFact03 , June 11, 2003
5.1 km
ConceptConceptConceptConceptMeasurement of Measurement of Measurement of Measurement of ννννµµµµ disappearance with a very large baselinedisappearance with a very large baselinedisappearance with a very large baselinedisappearance with a very large baseline
• UNK tunnel - huge scintillator based muon counter (not calorimeter !)• Surrounding soil is a neutrino target• TOF and segmentation gives direction to the neutrino source• Location at 50 m underground gives good cosmic ray background suppression• Energy scan with Narrow Band neutrino beam to see oscillation pattern
UNK tunnel(Left from terminated accelerator
project at the IHEP, Protvino, Russia)
Y. Efremenko
~~~~1 Mton
Fermilab ~~~~7600 kmJHF ~~~~7000 kmGSI ~~~~2000 km
WG1 SummaryNuFact03 , June 11, 2003
For ∆∆∆∆matm2 in the range of
1.5 10-3 ev2 < ∆∆∆∆m2 < 4.0 10-3 ev2
Expected accuracy in parameters measurementsFor GSI: σσσσ∆∆∆∆m2 = 2.7⋅⋅⋅⋅10-5 ev2 , σσσσSin22θθθθ = 0.01 For JHF: σσσσ∆∆∆∆m2 = 1.5⋅⋅⋅⋅10-5 ev2 , σσσσ Sin22θθθθ = 0.01
This is ~1% error !!!
If we can do the same for antineutrinos say with 2% accuracy, then:
Test of CTP on the 3% level by compare ∆∆∆∆m2 for neutrinos with∆∆∆∆m2 for antineutrinos
Sensitivity to matter effects on the 3% levelFor ∆µ∆µ∆µ∆µ = P(ννννµµµµ ) -- P(anti-ννννµµµµ )
Expected SensitivityExpected SensitivityExpected SensitivityExpected Sensitivity
WG1 SummaryNuFact03 , June 11, 2003
Detector: 30 kt magnetized iron calorimeter
Phase 1: atmospheric neutrino measurements
Phase 2: far detector for a neutrino factory experiment
WG1 SummaryNuFact03 , June 11, 2003
CERN
Fermilab
JHF
WG1 SummaryNuFact03 , June 11, 2003
(“super-beam”) LBL experiments
0.2%
0.4%
0.5%
0.5%
0.2%
0.2%0.2%0.2%0.2%
0.8%
1.2%
~1%
νe@peak
~4,000?20kt?730?~2OA1.2120OA-NuMI2
~400
650(0)
~1,000?
~2,500?
~600,000
~3,000~3,000~3,000~3,000
~5,000
~2,500
~50
νµCC(/yr)
1,0002950.7OA450JHF-HK
1,000?2,500?~1WB/OA
1.328AGS ??
1,000?~12000.8OA0.3400OA-CNGS
40(400)1300.26WB42.2SPL-Furejus
50kt?730?~2OA0.4120OA-NuMI
22.522.522.522.5
~2
5.4
22.5
Mdet
(kt)
295295295295
732
730
250
L(km)
〈Eνννν〉
(GeV)Beam
Power
(MW)Ep
(GeV)
0.70.70.70.7OAOAOAOA0.750.750.750.7550505050JHFJHFJHFJHF----SKSKSKSK
18WB0.3400CNGS
3.5WB0.41120MINOS(LE)
1.3WB0.00512K2K
T. Kobayashi, NuFact 02 (with modification for OA-NuMI)
WG1 SummaryNuFact03 , June 11, 2003
Future Experiments: Summary
CNGS: First beam May 2006
OPERA: Preparing for Day 1
ICARUS: T600 installation in Gran Sasso 2003 - 2004
JHF: Ready to start construction in 2004
NuMI off-axis: Detector choice advanced,
Proposal November 2003
BNL/Homestake: Realistic BG estimate suggested
IHEP, INO detectors: New comers welcome,
Realistic sensitivity studies encouraged