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1
J-PARC and T2K
1. Accelerator construction status and commissioning
2. Accelerator upgrade plan in first 5 years
3. Experiments with slow extracted beam
4. The T2K experiment
5. Possible future experiment
6. Summary
IV International Workshop on: “Neutrino Oscillations in Venice”
April 18, 2008Koichiro Nishikawa (KEK)
2
Materials and Life ScienceExperimental Facility
Hadron Beam Facility
Nuclear Transmutation
J-PARC
J-PARC = Japan Proton Accelerator Research ComplexJoint Project between KEK and JAEA
3 GeV Synchrotron(25 Hz, 1MW)
Linac
(350m)
50 GeV Synchrotron
(0.75 MW)
500 m
Neutrino to Kamiokande
Slow Extracted Beam Facility
3
Linac
SDTL
Ion source, LEBT, RFQ, MEBT(2 choppers, 2 bunchers)
Not funded Second phase
DTLFront-end part
• Particle: H-
• Energy: on day-one 181 MeV with ACS 400 MeV • Peak current:
at 181 MeV 30 mA at 400 MeV 50 mA • Repetition: 25 Hz • Pulse width: 0.5 msec
Commissioned Jan.2007 upto SDTL ( 181 MeV )
4
Excellent stability of LINAC
Parameter Unit Design Commissioninggoal *
Achieved to date
Output energy MeV 181 181 181Peak current mA 30 25 25 30 (RFQ)Linac beam power kW 36 1.2 1.2 (w/o chop)Momentum spread % < ± 0.2
includig jitter< ± 0.2includig jitter
25 mA:0.16 (FWHM)
Orbit distorsion mm ± 1 ± 1 ± 1Beam position jitter mm ± 0.1 ± 0.1 ± 0.2**Peak current fluctuation % ± 1 ± 1 ± 1***
Values in gray are preliminary.
** During several hours.*** During several hours. With the peak current and pulse width of 25 mA and 0.25 ms,
* Corresponding to 20 kW beam power from RCS
M. Ikegami, ATAC2008
5
Status of RCS (Commissioned Nov 2007)
Collimator section
RF section
Beam injection section
Circumference 348 mRepetition rate 25 HzInjection energy 181/400 MeVExtraction energy3 GeVHarmonic number 2
RF section
from Linac to MLF
RCS
to MR
1st arc sectionTwo beam transport lines
3NBT:transport line to the MLF3-50BT: transport line to the MR
3NBT
3-50BT
MR
MLF
Injection section Extraction section
6
Qx
Qy
(6.35,6.47)
(6.64,6.25)
~3.8x10^11 /bunch (Peak: 22mA, Macro: 0.05ms, Medium: 112ns, Vrf~420kV)~1.9x10^12 /bunch (Peak: 22mA, Macro: 0.05ms, Medium: 560ns, Vrf~420kV)~3.8x10^12 /bunch (Peak: 22mA, Macro: 0.1ms, Medium: 560ns, Vrf~420kV)~4.6x10^12 /bunch (Peak: 22mA, Macro: 0.12ms, Medium: 560ns, Vrf~440kV)
Measured for h=2, 1-bunch op.w/o painting injection
~3.8x10^11 /bunch
~1.9x10^12 /bunch
~3.8x10^12 /bunch
~4.6x10^12 /bunch
“~4.6x1012/bunch; h=2, 1bunch; 25Hz ” operation Successfully performed !!!!!
5Qy=31?
2Qy=13
2Q
x=
13
Q x-Qy=0
Q x-2Q y
=-6
Qx +Q
y =13
corresponding to100 kW in terms of particles per bunch
~6.5% loss near the injection : ⇒ ~0.42kW (assuming 2-bunch op.) <4kW (collimator limit)
Current dependence of the beam loss
H. Hotchi, ATAC2008
7
Summary of Linac/RCS status
• The linac and RCS have been commissioned successfully.• The stability of linac beam is sufficiently good for beam com
missioning of RCS. For RCS:- The optics measurement and its correction were successfully
performed.- The acceleration of 4.6x1012 particles (h=2, 1bunch) with 25
Hz repetition , corresponding to 100 kW operation in terms of particles per bunch, has been achieved.
- The particle loss was almost localized on the collimators.
- The RCS is ready for the MR & MLF beam commissioning- NEXT(Now) : Painting in injection
8
MR (slow cycling Main Ring synchrotron)
RCS
InjectionSlow extraction
Fast extraction
Neutrino beamline
Rf cavities
Beam abort lineHadron Experimental Hall
3-50 BT
To Super-Kamiokande
Ring collimators
BTcollimators
Hadron beamline
Circumference 1567.5 mRepetition rate ~ 0.3 HzInjection energy 3 GeVExtraction energy 30 GeV (start)Superperiodicity 3h 9No of bunches 8 (6 in 2009)Transition j 31.7Transverse emittanceAt injection ~54 mm-mradAt extraction ~10 mm-mrad(30 GeV)
598 ns
58 ns
4.2 s (8 bunches)
4x1013 Protons
9
MR status and commissioning plan
• Installation of accelerator components and vacuum system completed.
• Off beam commissioning has been started in Dec. 2007
• Beam commissioning is scheduled from May 2008.
– 1st stage (May-June 2008): 3 GeV DC opetration
– 2nd stage (Dec. 2007-Feb. 2008): Acceleration to 30 GeV, abort dump, beam extraction to hadron beamline
– 3rd stage (April -June 2009): Beam extraction to neutrino beamline
– 2x1020 protons on the target by the 2010 summer shutdown. ( T2k can search below CHOOZ limit with e-appearance )
10
Intensity Upgrade
11
• Space charge limit Make larger phase space in RCS RF bucket Single bunch operation - longer bucket• Cycle time Faster acceleration with more RF power
12
Power Upgrade of Neutrino Beam (8 bunches/pulse)
MR 30 GeV
LINAC 181MeV
Cycle time 3.52 sec
4 1013 P/bunch
0.27MW
RCS h=1 Operation
Cycle time 1.92
8.3 1013 P/bunch
1MW
0.91MW
MR 30 GeV
LINAC 400MeV
Cycle time 1.92sec
8.3 1013 P/bunch
1.66MW
MR RF Upgrade
Cycle time=1.76
0.55MW
5% 8% 17%
( MR usage of RCS)
LINAC 400MeV
0.45MW
13
Some experiments at ‘slow extracted beam’
14
Slow Extracted Beam Lines
Handron Hall
Beam Dump
K1.8
K1.8BR
KL
30~50 GeV primary beam
Productiontarget (T1)
K1.8
KL
15
E05 Hyper nucleiNo.1 priority in nuclear physics
2 MeV FWHM resolution
~6 events/day/MeV for 50 msr,
2g/cm2-thick Pb ~20 days
1616
Measurement of KMeasurement of KL L →→
17
E14 • Step 1
– Goal: First observation of the decay– Upgrade KEK E391a detector– New CsI (FNAL) calorimeter– 160 production angle (small neutron halo)– Beam survey in 2009
• ( Step 2: >100 events to measure the BR )
10-6
10-7
10-8
10-9
10-10
10-11
10-12
10-13
10-5
BR
Standard ModelStep 1
KEK E391a Run2
New Physics
18
-e conversion
Feasibility study•Extinction factor 10-9
•Fast kicker•SC near primary beam
Goal : 5x10-17
Predictions from SUSY Seesaw Models
with upgrade
19
• Current result is 3.4 sigma above from the SM value
• Efforts toward a proposal have started to realize the experiment in the earlier phase of J-PARC– Technical feasibility of bunch s
equences and beamline are being explored
– Harmonics changes in the MR and kicker design are key issues
– KEK designed new inflector for a better muon injection eff.
– g-2 ring to be shipped from BNL
Muon g-2@J-PARC
20List of ExperimentsMany nuclear physics experments
2121
T2K Collaboration~400 members from 12 Countries
Canada, France, Germany, Italy, Japan, Korea, Poland, Russia, Spain, Switzerland, UK, US
• High intensity beam (~102xK2K) from J-PARC MR• Discovery of e appearance Determine 13
• Precision meassurement of disappearance 23, m232
22
#
295km
23
Super Kamiokande Rebuilt
24
100
0
0
0
010
0
0
0
001
1212
1212
1313
1313
2323
2323
321
321
321
cs
sc
ces
esc
cs
sc
UUU
UUU
UUU
Ui
ieee
0.68<sin2212<0.94 sin2 2sin2 2
Lepton mixing pattern ?
0 1.0
90% CL allowed values
sin22 13sin2sin2
25
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 NBBFairly independent on spectrum dist.
Narrow intense beam: Off-axis beamOsci. Prob. @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
26
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 for osc
illation pattern studies• E(rec.) requirement on e candidates
2. Analysis of water Cherenkov detector data has accumulated almost twenty years of experience
– K2K has demonstrated BG rejection in e search
3. Hadron production measurement (NA61)4. Neutrino interactions at similar energy region (SciBooNE)
27
• Measure prod. from Graphite target• 0-250mrad • 0.5-5GeV/c • K ratio • First data taking in Oct., 2007 (1month)
– Beam: 30GeV proton– Thin target (2cmt 4%int ):~ 500k int.– Replica target (90cm, 80%int): ~180k int.
• Measurements in 2008 planned
CERN-SPS NA61 (SHINE) experiment
T2K goal w/ NA61
(Nbg) for e app. 10% <4%
(sin2223) 1% 0.5%
(m232)[10-4eV2] 1 0.15
28
28
SciBooNE @ FNAL (Jun2007~)SciBooNE @ FNAL (Jun2007~) cross section at sub GeV (~T2
K)• Total collected POT: 1. 46E20
• : 9.2E19 (goal: 1E20)• : 5.4E19 (goal: 1E20)
(from K2K)
(from K2K)
CCQE cand
CCQE cand
Intensive analysis in progres on various modes
29
Beam MonitorProton beam to
Target
NA61K production
distribution
SciBooNENeutrino
interactions
Near detector observables
SKobservables
Fnear(E) Ffar(E)
• Measurements are product of ’s times ’s• K production & neutrino/antineutrino interaction model
30Erec(GeV)
Signal+BGSignal+BG
BGBG
0 1 2 30
10
20
30
40
Sensitivity: Sensitivity: ee appearance appearance
Discovery ofe appearance (,m)
(Pe, e)
E
e
p
e
4
OA2o 5years
m2 = 3x10-3eV2
sin2213 = 0.1
CHOOZ90%
>10 times improvement from CHOOZ
90%CL
31
La Thuile 2004
Measurement of sinMeasurement of sin , , mm
disappearance
m2 = 3.0 x 10-3 eV2
Fully contained , 1-ring, -like sample
# o
f ev
ents
(ar
b.
un
it)
w/o osc.
31
Stat. only
--68%CL (ln L=0.5)--90%CL (ln L=1.36)--99%CL (ln L=3.32)
Goal(sin22)~0.01
(m2)~<1×10-4
(OA2.5(OA2.5))
disappearance
32
Neutrino Beam Line and Near Detector
33
The T2K collaboration thanks CERN for allowing us to re-use UA1 magnet
34
Having been transported by lorry to Geneva La Praille and loaded onto freight trains that took them to the port of Antwerp (Belgium), the containers are now aboard container ships bound for Pusan in South Korea, from whence they will sail to the port of Hitachinaka, their point of entry to Japan.
Sailing... and has arrived at J-PARC site
35
Status of 280m Near DetectorsStatus of 280m Near DetectorsOn-axis detector(INGRID)
Iron+ScibarSandwich
In production, ready in Apr.2009
UA1 magnetbeing shippedInstalled in Apr-Jun.2008
Photo-sensor (~60k ch) in production TPCECAL
FGD
FGD
All are in production
36
MW Neutrino Beam Line
• Heating by dEdX
– Water cooling and He cooling (where possible)
• Shock wave and high radiation
– Remote handling
– Graphite for target and dump core (< 10ppm O2)
– Tritium, NOx production
– Minimum number of beam windows
One piece enclosure from entrance to the target area to beam dump, filled with He
37
37
p beam
horns
pions
target
To decayvolume
Iron shield
Concreteshield
He vessel
Target StationTarget Station
• Installation of the helium vessel(~470ton, 1000m3) finished, passed vacuum test in Nov. 2007 as scheduled
38
Target and hornsTarget and horns
38
p beam
3 horns (@ 320kA)
pions
target
To decayvolume
Iron shield
Concreteshield
He vessel
38
1st Horn3rd Horn
Graphite target (26mmx90cm)Day-1 target deliveredHelium gas cooling test successful
Long term test successful @ 320kAHorn1,3 for Day-1 delivered
Target inside Ti-alloy capusule
39
The Neutrino Facility in J-PARCThe Neutrino Facility in J-PARC
39
39
Preparation SectionPreparation Section
SC combined func magsSC combined func mags
Target-Horn SystemTarget-Horn System
Target StationTarget Station
Decay VolumeDecay VolumeBeam DumpBeam Dump
Final Final FocusingFocusingSectionSection
Muon MonitoriMuon Monitoring Pitng Pit
Near Neutrino DetectorNear Neutrino Detector
295km to 295km to Super-KamiokandeSuper-Kamiokande
110m110m
Construction: Apr. 2004 ~ Mar. 2009 (5yrs)
40
Conceptual Design
Engineering Design
Real Production Installation
Proton Beam monitor Feb.~
Superconducting magnets Feb~
Cryogenics Apr~
Normal Conducting magnets
Vacuum system
Target Aug.~
Horn Aug.~
Target Station
Beam Window Jul~
Decay Volume
Beam Dump Aug~
Muon monitor 08/09
Summary of StatusSummary of Status
• All components are in production phase• Installations are starting as scheduled
41
Beyond T2K
1986 Kamiokande
1996 SuperKamiokande K2K and T2K
2009 – MW neutrino beam New Detector
42
CP Violation in Lepton Sector Two approaches
E
LmmUUUU
E
LmmUUUUP
ij
ijjjii
ijjji
iji
2
)(sin)Im(2
4
)(sin)Re(4
22**
222**
CPV sin12 sin23 sin13 m212 (L/E) sin
Solar and Atmospheric
Second Max.
sinsin
2sin
E4
m
)(P)(P
)(P)(PA
13
12212
ee
eeCP
43
First / Second Maximum and
One of the most dangerous bias:Energy mis-reconstruction to lower value than real value
44
CPV in neutrino oscillation
• Depend on the size of different effects from various systematics
– Neutrino-Anti-Neutrino asymmetry
• Cross section, Detection efficiencies
• Ratios e differences
• Contamination of wrong sign
– First vs. Second Maximum
• Wide band beam (small off-axis beam)
• E (L) at the second maximum should be sufficiently large to have reasonable cross section (E≈0.5 GeV → L≈500km)
• Emeasurement over large range of energy (efficiency for low energy particles)
45
3 sensitivity for CPV in T2K
no BGsignal stat only
(signal+BG) stat only
stat+2%syst.stat+5%syst.
stat+10%syst.
CHOOZ excludedsin2213<0.12@m31
2~3x10-3eV2
T2K 3 discovery
3 CP sensitivity : ||>20o for sin2213>0.01 with 2% syst.
2MW, 1Mt2 yr for
6~7yr for
sinsin
2sin
E4
m
A
13
12212
CP
m212=6.9x10-5eV2
m322=2.8x10-3eV2
12=0.59423=/4
46
Some physics potential studiesSome physics potential studies
Presented by T.Maruyama @ NP08
Presented by K.Kaneyuki @ NP08
100kt Liq Ar TPC @ 660km/0.8deg, 5yr numu 0.54Mt W.C.@295km/2.5deg
SK full det sym w/ 5% syst
No syst, perfect energy reso.
47
SummarySummaryIn one year• J-PARC accelerator complex is being commissioned • Construction of T2K beam line is on time and will be commissioned in
April 2009• Aiming for first results in 2010
In several years• Plan for 1.66MW in 5 years
• T2K data taking which will provide vital information on , needed to define next step,
• Future detector R/D on Mt Water C /~100kt size LiqAr TPC at several candidate sites
Future• CPV in lepton sector and Proton Decay
48
Thank you for your attention
49
50
Primary proton beam linePrimary proton beam line• Superconducting Arc section
– 28 combined function magnets– D2.6T,Q18.6T/m, L=3.3m
• Normal conducting Preparation section and Final focusing (FF) section
– Installation in progress
5050
Tunnel completed (Dec. 2006)
26(/28) mags delivered11(/14) doubles installed
51
Secondary beam lineSecondary beam line
51
3NBT
6m厚コンクリート躯体
ディケイボリューム94m ビームダンプターゲットステーション
He vessel (470t,1000m3) completed, passed vac test in Nov. 2007
Beam dump graphite module being assembled
1/14 part
Sep, 2007
Mar. 2008DV under 3NBT installed in FY2005
52
Beta function and dispersion
: measured from the response
of the closed orbit for a dipole kick (STM)
Injection + Arc
Extraction + Arc
RF + Arc
s(m)
(m
)
Vertical, w/ kick angle corr.Horizontal, w/ kick angle corr.
Good agreement with the design.
181 MeV DC mode
s(m)
x(m
) y
(m)
Design
: Measured from rf-frequency dependenceof the closed orbit
H. Hotchi, ATAC2008
53
Intensity upgrade plan of the first three years 8 9 10 11 12 1 2 3 4 5 6 7 8 9 10 11 12 1 2 3 4 5 6 7 8 9 10 11 12 1 2 3
LINAC Output power <for RCS> kW 5.4<0.25> 5.4<0.6> 5.4<1.2>6 15 <18>
Peak current mA 5-25
Pulse width msec 50-100 50-250Beam Rep. pps single - 25 single - 25
RCS Output power kW 4 4 4 100 250 (280)(MLF) Typical Beam Rep. pps single - 25 single - 25single - 25
No. of Bunches 1 - 2 1 - 2 1- 2 1- 2 1- 2 2
Particles /bunch for MLF 4.2E11 4.2E11 8.5E11 4.2E12 1.1E13 1.2E13
Particles /bunch for MR (4.2E11) (4.2E11)
Particles /ring for MLF 8.3E12 2.1E13Particles /ring for MR (8.3E11) (4.2E11)
MR Output power kW 0.12 1.2 3.6 100
Energy GeV 3 30
Typical Beam Rep. pps 0.3 0.3 - 0.5
No. of Bunches 1 - 2 1 - 2 6 6
Particles /bunch 4.2E11 4.2E11 4.2E11 1.2E13Particles /ring 8.3E11 8.3E11 2.5E12 7.2E13
HD Output power kW 1.2
Energy GeV 30Particles /burst 8.3E11
NU Output power kW 3.6 100
Energy GeV 30Particles /burst 2.5E12 7.2E13
JFY 2008 JFY 2007 JFY2009
- Requirement from T2K: 2.0E20 protons on the target by the 2010 summer shutdown. - Guideline :Beam loss at each extraction point < 25 -100 W to keep residual radiation level < 1mSv/h.
54
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
(cf. 耐力 ~300 MPa)
Material heavier than Ti might be destroyed.
Cooling power and radiation shield 12GeV PS x 100
GPaTE 3
Residual radiation
> 1000Sv/h
55
Present Technology limit
• Temparature rise and thermal shock limit us about 2MW proton beam
– Alminum horn – Graphite target beam power
– Ti vacuum window number of protons
• Substantial R/D and experiences needed to go substantially beyond this limit
56
31322
132
232
132
13
212
13231223122
132
232
122
232
122
132
12
21313223131223122
13
21313223131223122313122
13
3122
232
132
13
sincos4
)21(8
sin)cos2(4
sinsinsinsin8
sinsincos)cos(8
sin4)(
E
aLSSSC
SSSCCSSSCCCS
SSSCCC
SSSCCSSSC
SSCP e
seigenvalue mass: ,
energy, neutrino: length,flight :
,4/
222
2
ijiij
ijij
mmmm
EL
ELm
Sij=sinij, Cij=cosij
e appearance probability
LE
L
GeV
E
cmgE
aL
2~
4][]/[6.7
4 3
CP conserving
CP
solar
matter effect
-, a -a for e
13
Small numbers•S31
•sinΦ21 ~ 0.03
mass hierarchy
57
Neutrino beam line with MW protons
57
•Shock wave
•Heat generation •Various sources including dE/dX 4kW(water), MW (air)
•magnets and their power water cooling•Target Horn TS-DV-BD wall /BD core water cooling
•Radioactive water and air•radioactive water 13GBq / 3weeks (must be diluted <30Bq/cc to dispose)
many tanks, ion exchange filter, backup loop radioactive He 7GBq / 3 weeks (must be diluted <5mBq/cc to dispose) Production cross section of Tritium in He is 1/10 of air He vessel ( need O2 <10ppm)