Super-Kamiokande
Super-Kamiokande
Super-Kamiokande
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May 26, 2006<br />
Vulcano Workshop 2006<br />
<strong>Super</strong>-<strong>Kamiokande</strong><br />
~The Status of n Oscillation ~<br />
Yoshihisa OBAYASHI<br />
(ICRR, Univ. of Tokyo)<br />
for <strong>Super</strong>-<strong>Kamiokande</strong> Collaboration<br />
May 26, 2006<br />
Y.Obayashi @ Vulcano 2006 1
News: SK is Fully Reconstructed!<br />
• Apr. 2006 All PMTs are mounted with<br />
acrylic/FRP covers and start water filling<br />
May 14: Celebration for SK 10 th<br />
anniversary and Commissioning<br />
of SK-III<br />
PMT with cover<br />
Many T2K collaborators took<br />
reconstruction shifts<br />
Now: Half of tank is filled with water<br />
• End of Jun. 2006: Filled with water and restart<br />
observation<br />
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
2
42 m<br />
<strong>Super</strong>-<strong>Kamiokande</strong><br />
• 50kton pure water (22.5kt fid.vol.)<br />
• 11200 (Inner detector) + 1800<br />
(Outer detector) PMTs<br />
• 1000m underground 2700m<br />
wat. eq.<br />
39.3 m<br />
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
3
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
4<br />
History<br />
1996<br />
1997<br />
1998<br />
1999<br />
2000<br />
2001<br />
2002<br />
2003<br />
2004<br />
2005<br />
2006<br />
2007<br />
2008<br />
Start<br />
SK-I<br />
SK-II<br />
SK-III<br />
# of PMT<br />
(Photo Coverage)<br />
11,146<br />
(40%)<br />
Accident<br />
Partial Reconstruction<br />
Full Reconstruction<br />
5,182<br />
(19%)<br />
11,129<br />
(40%)<br />
Energy Threshold<br />
(Solar n)<br />
5 MeV<br />
7 MeV<br />
4 MeV(plan)<br />
Major Physics<br />
Outputs<br />
Atm. n Oscilaltion<br />
Phys. Rev. Lett. 81,1562(1998)<br />
Solar n Oscilaltion<br />
Phys. Rev. Lett. 86,5651(2001)<br />
Atm. n L/E<br />
Phys. Rev. Lett. 93, 101801(2004)<br />
K2K Final Result
Overview<br />
Atmospheric Neutrinos<br />
nm disappearance analysis<br />
nm nt or other modes<br />
Solar Neutrinos<br />
SK-I results<br />
SK-II update<br />
Improvement for SK-III<br />
<strong>Super</strong>novae Neutrinos<br />
Summary<br />
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
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6<br />
Atmospheric Neutrinos<br />
p, He …<br />
Zenith angle<br />
Q<br />
Downward<br />
(L=10~100 km)<br />
Event<br />
Classification<br />
p ± , K ±<br />
m ±<br />
Fully Contained<br />
(FC) (E n ~1GeV)<br />
n m<br />
e ±<br />
Partially Contained<br />
(PC) (E n ~10GeV)<br />
n m<br />
n e<br />
Upward<br />
(L=up to 13000 km)<br />
Stopping m (E n ~10GeV)<br />
Through-going m (E n ~100GeV)<br />
Particle ID<br />
(Fully Contained)<br />
e- like mu- like
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
7<br />
Zenith Angle Distribution<br />
SK-I : 1489 days<br />
SK-II : 804 days<br />
n m –n t oscillation (best fit)<br />
null oscillation<br />
FC<br />
FC<br />
< <<br />
FC<br />
FC<br />
FC<br />
><br />
FC<br />
><br />
FC<br />
FC
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
8<br />
Oscillation Analysis<br />
m/e double ratio allowed region (n m n t )<br />
Update from<br />
Phys. Rev. D 72, 052007 (2005)<br />
(SK-I results)<br />
Sub-GeV<br />
SK-II :<br />
SK-I :<br />
( m / e)<br />
( m / e)<br />
DATA<br />
MC<br />
0.656<br />
0.022<br />
0.033<br />
0.658<br />
0.016<br />
0.035<br />
Best Fit: Dm 2 = 2.5 x 10 -3 eV 2<br />
sin 2 2q = 1.00<br />
c 2 = 839.7 / 755 dof (18%)<br />
Multi-GeV (FC+PC)<br />
( m / e)<br />
DATA<br />
0.047<br />
SK-II : 0.7460 .044<br />
0. 055<br />
( m / e)<br />
MC<br />
SK-I :<br />
0.702<br />
0.032<br />
0.030<br />
<br />
0.101<br />
1.9 x 10 -3 eV 2 < Dm 2 < 3.1 x 10 -3 eV 2<br />
sin 2 2q > 0.93 at 90% CL
L/E analysis<br />
Update from<br />
Phys. Rev. Lett. 93,101801(2004)<br />
•<br />
• Select good L/E resolution (
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
10<br />
L/E Analysis result<br />
Zenith angle binning<br />
Oscillation<br />
Decay<br />
Decoherence<br />
c 2 osc<br />
c 2 dcy<br />
c 2 dec<br />
= 83.9/d.o.f<br />
= 107.1/d.o.f, Dc 2 = 23.2(4.8σ)<br />
= 112.5/d.o.f, Dc 2 = 27.6(5.3σ)
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
11<br />
3 Flavor Oscillation<br />
Submitted to Phys. Rev. D,<br />
see hep-ex/0604011<br />
• In the case q 13 ≠0:<br />
ne excess may be seen<br />
• Matter effect enhance n e appearance<br />
vacuum<br />
matter<br />
nm ne oscillation probability,<br />
Dm 2 =2.5x10 -3 eV 2 ,<br />
sin 2 q 23 =0.5,<br />
sin 2 q 13 =0.04
3 Flavor Analysis Result<br />
• Excess of up-going ne<br />
– SK-I data shows<br />
no excess yet<br />
• Allowed region<br />
– Consistent with pure nmnt<br />
SK-I<br />
1489days<br />
Best fit<br />
(Dm 2 =2.5<br />
x10 -3 eV 2 ,<br />
sin 2 q 23 =0.5,<br />
sin 2 q 13 =0.0)<br />
Expected excess<br />
(Dm 2 =2.5x10 -3 eV 2 ,<br />
sin 2 q 23 =0.5,<br />
sin 2 q 13 =0.04)<br />
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
12
Tau Appearance Search<br />
• Tau Enrich Sample:<br />
– Evis>1.33GeV (Multi-GeV)<br />
– Most energetic ring is e-like<br />
– Likelihood selection<br />
• Visible Energy<br />
• Sphericity<br />
• Distance between n interaction and<br />
decay-e<br />
• Zenith angle fit with tau signal and<br />
nm background<br />
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n m n t or n sterile <br />
Admixture model:<br />
Consistent of 0% of n s ,<br />
Arrow ~25% of sterile<br />
at 90% CL
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
15<br />
Other than Oscillation<br />
LIV<br />
S.Coleman & S.L. Glashow PRD 59(116008),1999<br />
V.Barger et. al., PRL 85(24),2000<br />
2<br />
<br />
<br />
2 2<br />
Dm<br />
<br />
P OSC<br />
sin 2q<br />
sin 1.27<br />
2Db<br />
L<br />
E <br />
• Best fit: c2(377dof)=399,<br />
(a=0.053,sin2q v =0.093)<br />
• a
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
16<br />
Solar Neutrinos<br />
• 8 B neutrino – electron scattering n + e - → n + e -<br />
SSM Expectation<br />
Typical Solar n event<br />
5.94(1+/-0.01)x10 10 /cm 2 /s (BP04 SSM)<br />
5.79(1+/-0.23)x10 6 /cm 2 /s<br />
8<br />
B<br />
Ee = 9.1MeV<br />
cosqsun = 0.95
Solar n Data of SK-I<br />
May 31, 1996 – July 13, 2001 (1496 days )<br />
n + e - n + e -<br />
22400230 solar n events<br />
(14.5 events/day)<br />
8<br />
B flux : 2.35 0.02 0.08 [x 10 6 /cm 2 /sec]<br />
Data<br />
SSM(BP2004)<br />
= 0.406<br />
0.004<br />
+0.014<br />
-0.013<br />
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
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18<br />
n e and n m +n t Fluxes(SK and SNO Results)<br />
SK<br />
SNO<br />
ES = 2.350.09 [x10 6 /cm 2 /s]<br />
CC = 1.720.08<br />
ES = e +0.15 m,t<br />
CC = e<br />
SNO NC = 4.980.35 NC = e + m + t<br />
(cf. SSM(BS2005) = 5.69±0.93)<br />
Obtained total flux: exp = 5.2±0.3<br />
SK<br />
SNO CC<br />
SNO NC<br />
±<br />
(BS2005)
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
19<br />
Energy spectrum of SK-I<br />
(tan 2 q, Dm 2 )<br />
Energy correlated systematic error
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
20<br />
Solar n results from SK-I<br />
Region represents<br />
allowed values of<br />
neutrino properties
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SK-II Solar n data<br />
(Preliminary)
Energy Spectrum<br />
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P(n e → n e )<br />
E<br />
May 26, 2006 n (MeV)<br />
Y.Obayashi @ Vulcano 2006<br />
25<br />
Solar n @ SK-III<br />
n e survival probability<br />
Recoil electron spectrum<br />
To see ~10% spectrum distortion,<br />
Lower energy threshold<br />
Minimize statistic error<br />
Minimize systematic error<br />
sys. error<br />
sin 2 (q)<br />
0.35<br />
0.28<br />
0.28<br />
0.28<br />
0.22<br />
Dm 2 (eV 2 )<br />
6.3 x 10 -5<br />
4.8 x 10 -5<br />
7.2 x 10 -5<br />
10.0 x 10 -5<br />
7.2 x 10 -5
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Background from Radon @ SK-I<br />
Y.Takeuchi et al., PLB452(1999)418
Improvement<br />
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28<br />
<strong>Super</strong>nova Neutrino Bursts<br />
No candidate was found in SK-I and SK-II<br />
2.3<br />
T<br />
< 0.39 SN/yr (90%CL)<br />
Upper limit of galactic SN rate <<br />
Efficiency vs. Distance<br />
T: measurement time
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
29<br />
<strong>Super</strong>novae Relic Neutrinos<br />
Reactor n<br />
Solar 8 B<br />
Solar hep<br />
Expectations<br />
Population synthesis (Totani et al., 1996)<br />
Constant SN rate (Totani et al., 1996)<br />
Cosmic gas infall (Malaney, 1997)<br />
Cosmic chemical evolution (Hartmann et al., 1997)<br />
Heavy metal abundance (Kaplinghat et al., 2000)<br />
LMA n oscillation (Ando et al., 2002)<br />
Atmospheric n<br />
Phys. Rev. Lett. 90, 061101(2003)<br />
SK-I<br />
Total background<br />
Atmospheric n m →<br />
invisible m →<br />
decay e<br />
90% CL limit<br />
of SRN<br />
Atmospheric n e
Atmospheric Neutrinos<br />
Summary<br />
Oscillation analysis result based on SK-1 (1489d) +SK-<br />
2(890d) is presented<br />
Further analysis based on SK-I(1489d)<br />
Consistent with nm nt oscillation.<br />
Some non-tau modes: unlikely<br />
Solar Neutrinos<br />
Oscillation analysis based on SK-I(1469d) is presented<br />
SK-II data also analyzed though energy threshold is<br />
7MeV<br />
Improvements for SK-III is going on<br />
Upper limits for SN and SRN rate obtained<br />
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
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Supplements<br />
May 26, 2006<br />
Y.Obayashi @ Vulcano 2006 31
Tau Appearance Search<br />
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33<br />
Zenith Angle Distributions (SK-I bins)<br />
n m –n t oscillation (best fit)<br />
null oscillation
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
34<br />
Zenith Angle Distributions (SK-II bins)<br />
n m –n t oscillation (best fit)<br />
null oscillation
SK-I + SK-II combined analysis (data binning)<br />
P lep<br />
Sub-GeV Multi-GeV<br />
CC n e CC n m<br />
FC FC FC FC<br />
UP through<br />
PC PC<br />
1ring mring 1ring mring<br />
showering<br />
stop thru<br />
e-like e-like m-like m-like<br />
UP through<br />
non-showering<br />
38 event type and<br />
momentum bins<br />
UP<br />
x<br />
stop 10 zenith bins<br />
380 bins<br />
Since various detector related systematic errors are different,<br />
we do not combine the SK-I and SK-II bins.<br />
380 bins for SK-I + 380 bins for SK-II 760 bins in total
SK-I + SK-II combined analysis (systematic errors)<br />
neutrino flux (14)<br />
neutrino interaction (12)<br />
Identical for SK-I and SK-II<br />
solar activity (1)<br />
event selection<br />
and reconstruction (21)<br />
Regarded as independent<br />
between SK-I and SK-II<br />
The total number of systematic errors is :<br />
Flux (14) + Interaction (12) + SK-I (22) + SK-II (22) = 70
Result from SK-I + SK-II data<br />
SK-I : 1489 days<br />
SK-II : 804 days<br />
Best Fit: Dm 2 = 2.5 x 10 -3 eV 2<br />
sin 2 2q = 1.00<br />
c 2 = 839.7 / 755 dof (18%)<br />
1.9 x 10 -3 eV 2 < Dm 2 < 3.1 x 10 -3 eV 2<br />
sin 2 2q > 0.93 at 90% CL
SK+ K2K Combined Results<br />
K2K<br />
K2K<br />
Combine<br />
Combine<br />
SK<br />
SK<br />
Combined result sin 2 2q Dm 2 [eV 2 ]<br />
Best fit point 1.03 2.4910 -3<br />
Best in phys. 1.00 2.5110 -3<br />
Arrowed region of Dm 2 @<br />
sin 2 2q1<br />
2.29(-9%) ~ 2.84(+13%) [eV 2 ] (68%)<br />
2.17(-14%) ~ 3.03(+21%) [eV 2 ] (90%)<br />
May 26, 2006 Y.Obayashi @ Vulcano 2006<br />
38