long baseline neutrino experiment in japan
DESCRIPTION
Long Baseline Neutrino Experiment in Japan. T2K (Tokai to Kamioka Neutrino Oscillation Experiment) Neutrino facility becomes a reality in 3 years. III International Workshop on “Neutrino Oscillations in Venice” Koichiro Nishikawa Kyoto University February 8, 2006. J-PARC Facility. 500 m. - PowerPoint PPT PresentationTRANSCRIPT
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Long Baseline Neutrino Experiment in Japan
III International Workshop on “Neutrino Oscillations in Venice”
Koichiro NishikawaKyoto UniversityFebruary 8, 2006
T2K (Tokai to Kamioka Neutrino Oscillation Experiment) Neutrino facility becomes a reality in 3 years
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Materials and Life ScienceExperimental Facility
Hadron Beam Facility
Nuclear Transmutation
J-PARC Facility
J-PARC = Japan Proton Accelerator Research ComplexJoint Project between KEK and JAERI
3 GeV Synchrotron(25 Hz, 1MW)
Linac
(350m)
50 GeV Synchrotron
(0.75 MW)
500 m
Neutrino to Kamiokande
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Non-zero mass of neutrinos !What kind of neutrino facility needed for years to come? Flavor Physics esp. history of neutrino studies show full of surprises ⇔ co op with unexpected ( Kamiokande for Kamioka Nucleon decay Experiment ! )
Quantities: lepton ID and neutrino energy E
Good EdeterminationPrecision measurement of 23
Precision measurement of oscillation pattern⇒ oscillation + ?
Lepton ID, NC-CC distinctione -appearance m2 ⇒MNS 3gen. formulation like CKMe-appearance exp. ⇒CPV in leptonic process (leptogenesis?)
What is the best configuration for Eand PID, given detector must be massive (simple) ?
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Main features of T2K-1The distance (295km) and m2 (~2.5x10-3 eV2 )1. Oscillation max. at sub-GeV neutrino energy
– sub-GeV means QE dominant• Event-by event Ereconstruction
– Small high energy tail • small BKG in e search and Ereconstruction
2. Proper coverage of near detector(s) – Cross section ambiguity
3. Analysis of water Cherenkov detector data has accumulated almost twenty years of experience
– K2K has demonstrated BG rejection in e search– Realistic systematic errors and how to improve
4. Accumulation of technologies on high power beam
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~1GeV beam(100 of K2K)
Tokai
Physics goalsDiscovery ofe appearance Precise meas. of disappearancex
Kamioka
J-PARC0.75MW 50GeV PS
Super-K: 50 ktonWater Cherenkov
Phase2:3~4 MW
Phase2:Hyper-K
Long baseline neutrino oscillation experiment from Tokai to Kamioka. (T2K)
12 countries~60 institutions
~180 collaboratorsDiscovery of CP violation (Phase2)
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E reconstruction at low energy
CC QE can reconstruct Ep
bkg. for E measurement
High energy part
bkg.for e-appearance
+ n → + p
-
p
(E, p)
+ n → + p + ’s
p’s
-
+ n → + p +
p
(E, p)
’s
cospEm
2mEmE
N
2Nrec
E MeV E/E ~ 10%
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1. Beam energy • Only the product F(E) x (E) is observable spectrum changes by oscil.
– Sub-GeV small HE tail – CCQE dominates (1 process)
• Even QE absolute cross section is known only with 20-30% precision– measurements at production
with similar spectrum are critical
• Intermediate energy flux should be kept to minimum– Many processes contribute (Q
E, 1DIS)– Spectrum changes causes mix
ture of processes changes
1 10 E
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TargetHornsDecay Pipe
Super-K.
decay Kinematics
OA3°
OA0°OA2°
OA2.5°
Statistics at SK (OAB 2.5 deg, 1 yr, 22.5 kt)
~ 2200 tot ~ 1600 CC e ~0.4% at peak
Quasi Monochromatic Beam x 2~3 intense than NBBTuned at oscillation maximum
Narrow intense beam: Off-axis beam振動確率@m2=3x10-3eV2
f
lux
0°
2°
2.5°3°
E (
GeV
)
1
00 2 8
p (GeV/c)5
Anti-neutrinos by reversing Horn current
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Main features of T2K-1The distance (295km) and m2 (~2.5x10-3 eV2 )
1. Oscillation max. at sub-GeV neutrino energy
– sub-GeV means QE dominant
• Event-by event Ereconstruction
– Small high energy tail
• small BKG in e search and Ereconstruction
2. Proper coverage of near detector(s) – Cross section ambiguity
3. Analysis of water Cherenkov detector data has accumulated almost twenty years of experience
– K2K has demonstrated BG rejection in e search
– Realistic systematic errors and how to improve
4. Accumulation of technologies on high power beam
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• Neutrino cross section cannot be trusted above GeV and below deep inelastic region –
• Proper near detectors to measure rate and Far/Near ratio should be used
Experiences in K2K with Harp measurement
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• Muon monitors @ ~140m– Fast (spill-by-spill) monitoring of b
eam direction/intensity (→• First near detector @280m
– Flux/spectrum/e - off-axis– intensity/direction - on-axis
• Second near detector @ ~2km– Almost same E spectrum as for S
K– facility request after commissionin
g of beam line• Far detector @ 295km
– Super-Kamiokande (50kt)
1.5km
295km
0.28km
Neutrino spectra at diff. dist
p
140m0m 280m 2 km 295 km
2. Near detector complexNot approved yet
1 2 3 EGeV
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Conceptual Design of Near Detector @ 280m
Magnet + Side-MRD
Magnet + Side-MRD
P0D TPC TPC TPCFG
D
Pb-
P0D
EM calorimeter
EM calorimeter
EM
ca
lori
me
ter
Mu
on
ID h
odos
cope
FG
D+
H2O
3m1m
1m
PMT
Iron
Tracker : SciBar type Extruded Scintillator + Wave Length Shifting Fiber
Veto all surface by plastic scintillator (Fibers goes through holes.)
3m
1m
1m
20m
36m
3
2
5m
FGDMRD
~14m
SK
beam
20m
36m
3
2
5m
FGDMRD
~14m
SK
beam
• Off-axis detector spectrumCross sect.e contami.UA1 mag, FGD, TP
C, Ecal,..• On axis detectorMonitor beam dir.Grid layout
On-axis
Off-axisDetectorHole
UA1 mag
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Possible 2km detectors
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Main features of T2K-1The distance (295km) and m2 (~2.5x10-3 eV2 )
1. Oscillation max. at sub-GeV neutrino energy
– sub-GeV means QE dominant
• Event-by event Ereconstruction
– Small high energy tail
• small BKG in e search and Ereconstruction
2. Proper coverage of near detector(s)
– Cross section ambiguity
3. Analysis of water Cherenkov detector data has accumulated almost twenty years of experience
– K2K has demonstrated BG rejection in e search– Realistic systematic errors and how to improve
4. Accumulation of technologies on high power beam
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3. PID in SK e-like -like
e
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Particle ID (e & ) (in single ring events)
• An experiment with test beams confirmed the particle ID capability (PL B374(1996)238)
Super-KamiokandeAtmosphric data
e
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K2K 1KT data and MC reproducibility
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SK data reduction in K2K real data:―K2K-1― MC beam e Data
FCFV 79.7*1 0.80 55
Single ring 49.97 0.46 33
Electron like*2 2.62 0.40 3
Evis > 100 MeV 2.43 0.39 2
No decay-e 1.88 0.34 1
Pi0 cut 0.57 0.17 0
*1 Normalized by Nsk*1 Normalized by Nsk*2 different from std. PID*2 different from std. PID (opening angle & ring patter(opening angle & ring pattern)n)
―K2K-2― MC beam e Data
FCFV 76.2*1 0.85 57
Single ring 48.52 0.51 34
Electron like*2 3.17 0.44 5
Evis > 100 MeV 2.89 0.44 5
No decay-e 2.14 0.38 4
Pi0 cut 0.73 0.21 1
In total,In total, #expected BG = #expected BG = 1.681.68 #observed = #observed = 11
NC BKG 1.3 events
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Search for e oscillation in K2K has achieved necessary rejection
•K2K real data with background rejection algorithmAs a result, # of expected BG 1.68 events
(1.3 from & 0.38 from beam e) # of observed events 1 event
1/3 by HE tail – NC 1/3 by E rec
Rough extrapolation to T2Kx~100 without osc.Shown by real data
BKG ~1.3x100/9~15 for 5 years T2K
T2K low energy beam, small tail
e
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Sensitivities, precision in T2K phase-1
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Disappearance Ereconstruction resolution
Large QE fraction for <1 GeV Knowledge of QE cross sections Beam with small high energy tail
QE
inelastic
E~60MeV<10% meaurement
E(reconstructed) – E(true)
1-sin22
non-QEresolution
m2
+ 10% bin High resolution : less sensitive to systematics
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Precision measurement of 23 , m223
possible systematic errors and phase-1 stat.•Systematic errors
• normalization (10% ( 5%(K2K))• non-qe/qe ratio (20% (to be measured))• E scale (4% (K2K 2%))• Spectrum shape (Fluka/MARS →(Near D.))• Spectrum width (10%)
OA2.5o
(sin22)~0.01 (m2
23) <1×10-4 eV2
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e appearance :
sin2213
Estimated background in Super-K Signal
(~40% eff.)
Signal + BG
NC
e
beam e total
0.1 12.0 10.7 1.7 0.5 24.9 114.6 139.5
0.01 12.0 10.7 1.7 0.5 24.9 11.5 36.4
sin2213
m2
Off axis 2 deg, 5 years
Off axis 2 deg, 5 yearsat
sin2213>0.006 C
HO
OZ
exc
lud
ed
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Sensitivity to 13 as a fuction of CP-phase
KASKA 90%(NuFact04)
KASKA 90%(NuFact04)
→- for →anti-
sin22
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Status of JPARC
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26Beam Test
0.2
0.0
MW
1.0
0.8
0.6
0.4
JFY2007
平成23年度 平成24年度平成19年度 平成20年度 平成21年度 平成22年度
Usage for Experiments
Usage for Experiments
Usage for Experiment
3 GeVNeutron and Muon Construction
Construction
Construction
KEK PSPower
Completion of200 MeV Linac
400 MeV Linac Construction
200 MeVon Day 1
Expected Beam Power at 3 GeV
400 MeVon Day 1
400 MeV installationin 2008-2010
JFY2008 JFY2009 JFY2010 JFY2011 JFY2012
Completionof T2K
50 GeVNuclear - Particle
T 2 K Experiment
T2Kconstruction
3 GeV RCS commissioning plan
What aboutMR intensity?
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Intensity of MR• J-PARC start with 180 MeV LINAC
Currently, following realistic scenarios have been studied• Intensity in 3 GeV Booster limited by space charge effect
– increase number of bunches in MR by RF freq. increase in MR (injection time)
– larger bucket in Booster to increase no. of protons/bunches
– More RF power to increase rep. (with money)• Every possible effort to increase MR intensity faster than 3Ge
V booster
• Badget request will be submitted to restore 400 MeV LINAC (2008,9,10 ?)
• Eventually more than MW beam
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OR single bunchlarger bucket (protons/bunch larger)keep h=9 (rep. rate is same as original
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Accelerator commissioning planw/ LINAC upgrade
0
500
1000
1500
2000
2500
3000
2008 2008.5 2009 2009.5 2010 2010.5 2011 2011.5 2012 2012.5 2013J FY
Beam
pow
er (k
W)
RCS power
MR power
MR powerx2 Np
MR powerx2 Npx1.5 rep rateMR powerx2 Npx2 rep rate
Be
am P
ow
er
(MW
)
0
1
2
3
Japanese Fiscal Year (Apr-Mar)
2008 2009 2010 2011 2012
Need upgrades of beam line elements
RCS power
h.n.RF mod
h.n.+RFx2
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Main features of T2KThe distance (295km) and m2 (~2.5x10-3 eV2 )1. Oscillation max. at sub-GeV neutrino energy
– sub-GeV means QE dominant• Event-by event Ereconstruction
– Small high energy tail • small BKG in e search and Ereconstruction
2. Proper coverage of near detector(s) – Cross section ambiguity
3. Analysis of water Cherenkov detector data has accumulated almost twenty years of experience
– K2K has demonstrated BG rejection in e search– Realistic systematic errors and how to improve
4. Accumulation of technologies on high power beam handling
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First high enrgy MW fast-ext’ed beam !
cm
cm
1100o
(cf. melting point 1536o)
3.3E14 ppp w/ 5s pulse
When this beam hits an iron block,
Material heavier than iron would melt.
Thermal shock stress
(max stress ~300 MPa)
Material heavier than Ti might be destroyed.
GPaTE 3
Residual radiation
> 1000Sv/h
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decay volume
Near detector
TargetStation
Beam dump/-pit280m
130m
Neutrino Beam Line for T2K ExperimentSpecial FeaturesSpecial Features
Superconducting Superconducting combined combined
functionfunction magnets magnets
Off-axis beamOff-axis beam
ComponentsComponents Primary proton beam line
Normal conducting magnets
Superconducting arc
Proton beam monitors
Target/Horn system
Decay pipe (130m) Cover OA angle 2~3 deg.
Beam dump
muon monitors
Near neutrino detector
Construction: JFY2004~2008To Super-Kamiokande
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Schedule of T2K
• Possible upgrade in future →Next speaker– 4MW Super-J-PARC + Hyper-K ( 1Mt water
Cherenkov)– CP violation in lepton sector– Proton Decay
2004 2005 2006 2007 2008
SK full rebuild
T2K construction
April 2009commissioning
K2K
2009
Linac
MR
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Many new concepts emerged from studies of neutrinos.
LH worldQuark as physical constituentNumber of generationsWide variety mass of elementary particles…….
Tradition will continue and Tradition will continue and New results in 2010New results in 2010
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