hiroyuki sekiya ichep2014 jul. 4 2014 @valencia, spain solar neutrinos in super-kamiokande ichep2014...

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Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University of Tokyo for the Super-K Collaboration

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Page 1: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Solar Neutrinos inSuper-Kamiokande

ICHEP2014 @Valencia July 4 2014

1

Hiroyuki SekiyaICRR, University of Tokyo

for the Super-K Collaboration

Page 2: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

50kton pure water Cherenkov detector

1km (2.7km w.e) underground in Kamioka

11129 50cm PMTs in Inner Detector1885 20cm PMTs in Outer Detector

~3.5 ~20 ~1

Solar ν

MeV

Relic SN ν

GeV TeV

Atmospheric ν

~100

Physics targets of Super-Kamiokande

Proton decay

Super-Kamiokande

2

WIMPs

Page 3: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain 3

neSolar neutrinos observation

Super-K

n + e- n + e-

Page 4: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

The results: Solar global fit This SK update and other latest results are combined.

4

~2σ tension in Δm221

between solar and KamLAND

Solar

KamLAND

Solar+KamLAND

Reactor

preliminary

Non-zero q13 at 2 s from solar+KamLANDGood agreement with Daya Bay, RENO & DC (Neutrino2014)

Without reactor θ13 constraintCombined solar fit with KamLAND

sin2θ13=0.0242±0.0026

KamLANDSolar+KamLAND

Solar

sin2θ13=0.0221±0.0012

Page 5: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Motivation

Vacuum oscillation dominant

Matter oscillation dominant

up-turn!

Search for the direct signals of the MSW effect

Neutrino survival probability

Solar matter effect

Energy spectrum distortionEarth matter effect

Flux day-night asymmetry

5

Solar+KamLANDsin2θ12=0.308Δm2

21=7.50x10-5eV2

sin2θ12=0.311Δm2

21=4.85x10-5eV2

Solar

Regenerate ne by earth matter effectJHEP 0311:004(2003)

Page 6: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Improvements in SK-IV Reduced 222Rn BG

6

SK-III SK-IV

Achieved 3.5 MeV(kin.) energy threshold 8.6s signal is observed with MSG

Reduced systematic error 1.7% for flux cf. SK-I: 3.2% SK-III: 2.1%

4.0-4.5 MeV bin

New analysis in low energy bins Remaining BG-electrons from 214Bi should have more multiple-scatterings than signal-electrons have: MSG

3.5-4.0MeV

4.0-4.5MeV

MSG < 0.35 0.35<MSG<0.45 0.45<MSG

Page 7: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

8B solar n in SK-I+II+III+IV8B n signals

7

~70k solar neutrino events

8B n could be the BG for DM searchthrough NC coherent scattering.

FSK(8B) =2.344±0.034 x 106   cm-1s-1

preliminary

FSK+SNO(8B) =5.30 x 106   cm-1s-1+0.17

-0.11

preliminary

Page 8: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Recoil electron spectra

8

Dat

a/M

C(u

nosc

illat

ed)

preliminary

Kinetic energy (MeV)

Page 9: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

SK-I+II+III+IV spectrum

9

N.B. All SK phase are combined without regard to energy resolution or systematics in this figure

Neutrino energy spectrum is convoluted in the electron recoil spectrum. For de-convolution, generic functions are used as a survival probability;

Solar+KamLANDsin2θ12=0.308 Δm2

21=7.50x10-5eV2

Solarsin2θ12=0.311 Δm2

21=4.85x10-5eV2

SK recoil electron spectrum constrain the fit parameters (ci,ei) of the function and the allowed Pee(En) is derived using the allowed (ci,ei).

f8B=5.25 x 106/(cm2∙sec)

fhep=7.88 x 103/(cm2∙sec)

(total # of bins of SKI - IV is 83) χ2

Solar+KamLAND 70.13

Solar 68.14

quadratic fit 67.67

exponential fit 66.54

Page 10: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Allowed Pee(En) for SK

10

SK

Solar+KamLAND

Solar

✓MSW (solar+KamLAND) is consistent at ~1.6σ✓MSW (solar) fits better (at ~0.7σ)

sin2θ12=0.308Δm2

21=7.50x10-5eV2

sin2θ12=0.311Δm2

21=4.85x10-5eV2

preliminary

Page 11: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Allowed Pee(En) for SK+SNO

11

SK+SNOSNO

SK

Solar+KamLAND

Solar

✓SK and SNO are complementary for the shape constraint✓MSW is consistent at 1σ

sin2θ12=0.308Δm2

21=7.50x10-5eV2

sin2θ12=0.311Δm2

21=4.85x10-5eV2

preliminary

Page 12: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Global view of Pee(En)

12

SK+SNO

Borexino (8B)

all solar (pp) Borexino (pep)

Borexino (7Be)

Homestake+SK+SNO

(CNO)

preliminary

Page 13: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain 13

Earth

θz

Solar best fit

Solar+KamLAND

preliminary

SK-I - IV combined (Eth=4.5 MeV for SK-I,III,IV 6.5 MeV for SK-II)

sin2θ12=0.308Δm2

21=7.50x10-5eV2

sin2θ12=0.311Δm2

21=4.85x10-5eV2

Sun

Flux zenith angle distribution

Page 14: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Day/Night asymmetry amplitude

Fitted asymmetry amplitude

Δm221=4.84x10-5 eV2 Δm2

21=7.50x10-5 eV2

SK-I -2.0±1.8±1.0% -1.9±1.7±1.0%

SK-II -4.4±3.8±1.0% -4.4±3.6±1.0%

SK-III -4.2±2.7±0.7% -3.8±2.6±0.7%

SK-IV -3.6±1.6±0.6% -3.3±1.5±0.6%

combined -3.3±1.0±0.5% -3.1±1.0±0.5%non-zero

significance 3.0σ 2.8σ

14

Rat

e/R

ate a

vera

ge

expected

preliminary

Δm221=4.84x10-5 eV2

sin2θ12=0.311 sin2θ13=0.025

Energy-dependence of the variation

First observation of day/night asymmetry at 3s significance level

Page 15: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Δm221 dependence

15

sin2θ12=0.311, sin2θ13=0.025

1σ KamLAND1σ Solar

SK-I,II,III,IV best fit

expected2.8σ2.9σ3.0σ

Solar regiondiffer from zero by 2.9~3.0σagree with expect by 1.0σ

differ from zero by more than 2.8σagree with expect by 1.3σ

KamLAND region

preliminary

Page 16: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Summary

SK has observed ~70000 solar n interactions, by far the largest sample of solar neutrino events in the world.

SK data provide the first indication (at 2.8~3.0 s) of terrestrial matter effects on 8B solar n oscillation.

SK gives the world’s strongest constraints on the shape of the survival probability Pee(Eν) in the transition region between vacuum oscillations and MSW resonance.◦ SK spectrum results are consistent with MSW up-turn prediction

within ~1s. SK measurements strongly constrain neutrino oscillation parameters:

◦ SK gives world’s best constraint on Δm212 using neutrinos.

◦ There is a 2s tension between SK’s neutrino and KamLAND’s anti-neutrino measurement of Δm21

2. Last month SK started taking data at ~2.5 MeV at ~100% trigger

efficiency. Stay tuned for very low energy SK neutrino.

16

Page 17: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Extra slides

17

Page 18: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Full summary

SK has observed ~70000 solar neutrino interactions in ~4500days (1.5 solar cycles), by far the largest sample of solar neutrino events in the world.

SK data provide the first indication (at 2.8~3.0 sigma) of terrestrial matter effects on 8B solar neutrino oscillation. This is the first observation using a single detector and identical neutrino beams that matter affects neutrino oscillations.

SK has successfully lowered the analysis threshold to ~3.5 MeV kinetic recoil electron energy. SK gives the world’s strongest constraints on the shape of the survival probability Pee(Eν) in the

transition region between vacuum oscillations and MSW resonance. SK spectrum results slightly disfavor the MSW resonance curves, but are consistent with MSW

prediction within 1-1.7 sigma. SK measurements strongly constrain neutrino oscillation parameters: SK uniquely selects the Large Mixing Angle MSW region by >3sigma, gives world’s best constraint on solar Δm2 using neutrinos, and significantly contributes to the measurement of the solar angle. There is a 2 sigma tension between SK’s neutrino and KamLAND’s anti-neutrino measurement of

the solar Δm2. Last month SK started taking data at ~2.5 MeV at ~100% trigger efficiency. Stay tuned for very

low energy SK solar neutrino

18

Page 19: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Wide-band Intelligent Trigger Reconstruction and Reduction just after Front-end

19

Just started

100% trigger efficiency above 2.5MeV(kin.)

Page 20: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Oscillation parameter

20

Page 21: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain 21

Page 22: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Improvements in SK-IV Reduced BG

22

SK-III SK-IV

achieved 3.5 MeV(kin.) energy threshold

7.5s level signal is observed at 3.5MeV bin

Event rate becomes low and stable in SK-IV

Reduced systematic error 1.7% for flux cf. SK-I: 3.2% SK-III: 2.1%

4.0-4.5 MeV bin

Page 23: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

significance of the signal

The MSG non-zero signal significance is 8.6 sigma (2.4129/0.2811)

3.5- 4.0 MeV Data/SSM=0.4596+0.0546-0.0535 Flux=2.4129+0.2866-0.2811

23

Page 24: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

SK+SNO 8B total flux For each oscillation parameter set there is a minimum chi2 and a 8B error

term describing the parabolic increase of the chi2 with deviations from the best chi2. The reduced chi2 vs. 8B flux is below. The jump is due to the relatively coarse grid in theta12.

5.30+0.17-0.11x10^6/(cm2 sec), which is a (+3%,-2%) error on the total 8B for SK+SNO compared to the 1.5% error of SK's ES flux by itself.

24

Page 25: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Systematic errors

Total 1.7 %

25

Source SK-IV flux(3.5-19.5MeV)

SK-III flux(4.5-19.5MeV)

energy scale +1.14, -1.16% ±1.4%

energy resolution +0.14, -0.08% ±0.2%

B8 spectrum +0.33, -0.37% ±0.2%

trigger efficiency ±0.1% ±0.5%

angular resolution +0.32, -0.25% ±0.67%

vertex shift ±0.18% ±0.54%

BG event cut ±0.36% ±0.4%

hit pattern cut ±0.27% ±0.25%

another vertex cut removed ±0.45%

spallation cut ±0.2% ±0.2%

gamma cut ±0.26% ±0.25%

cluster hit cut +0.45, -0.44% ±0.5%

BG shape ±0.1% ±0.1%

signal extraction ±0.7% ±0.7%

cross section ±0.5% ±0.5%

Page 26: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

8B solar n in SK-I+II+III+IV8B n signals

26

Page 27: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Data set for global solar analysis

SK:◦ SK-I 1496 days, spectrum 4.5-19.5 MeV(kin.)+D/N:Ekin>4.5 MeV ◦ SK-II 791 days, spectrum 6.5-19.5 MeV(kin.)+D/N: Ekin>7.0 MeV◦ SK-III 548 days, spectrum 4.0-19.5 MeV(kin.)+D/N: Ekin>4.5 MeV◦ SK-IV 1669 days, spectrum 3.5-19.5 MeV(kin.)+D/N: Ekin>4.5 MeV

SNO:◦ Parameterized analysis (c0, c1, c2, a0, a1) of all SNO phased. (PRC88, 025501 (2013))

◦ Same method is applied to both SK and SNO with a0 and a1 to LMA expectation Radiochemical: Cl, Ga

◦ Ga rate: 66.1±3.1 SNU (All Ga global) (PRC80, 015807 (2009))◦ Cl rate: 2.56±0.23 SNU(Astrophys. J.496, 505 (1998) )

Borexino: Latest 7Be flux (PRL 107, 141302 (2011)) KamLAND reactor : Latest (3-flavor) analysis (PRD88, 3, 033001 (2013)) 8B spectrum: Winter 2006 (PRC73, 73, 025503 (2006)) 8B and hep flux

27

The most up-to-date data are used

f8B=5.25 x 106/(cm2∙sec)

fhep=7.88 x 103/(cm2∙sec)

Page 28: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Day/Night

28

Amplitude fitStraight calc.(D-N)/((D+N)/2)Δm2

21=4.84x10-5 eV2 Δm221=7.50x10-5 eV2

SK-I -2.0±1.8±1.0% -1.9±1.7±1.0% -2.1±2.0±1.3%

SK-II -4.4±3.8±1.0% -4.4±3.6±1.0% -5.5±4.2±3.7%

SK-III -4.2±2.7±0.7% -3.8±2.6±0.7% -5.9±3.2±1.3%

SK-IV -3.6±1.6±0.6% -3.3±1.5±0.6% -4.9±1.8±1.4%

combined -3.3±1.0±0.5% -3.1±1.0±0.5% -4.1±1.2±0.8%non-zero

significance 3.0σ 2.8σ 2.8σexpected time variation as a function of cosθz

preliminary

(sin2θ12=0.311, sin2θ13=0.025)R

ate/

Rat

e ave

rage

α : day-night asym. scaling factor

Page 29: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

exponential parameterization

29

preliminary

✓SK spectrum, red : exponential, green : quadratic

Solar+KamLAND

Solar

sin2θ12=0.308Δm2

21=7.50x10-5eV2

sin2θ12=0.311Δm2

21=4.85x10-5eV2

Page 30: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

SK-I+II+III+IV spectrum

30

(total # of bins of SKI - IV is 83) χ2

Solar+KamLAND 70.13

Solar 68.14

quadratic fit 67.67

N.B. All SK phase are combined without regard to energy resolution or systematics in this figure

Neutrino energy spectrum is convoluted in the electron recoil spectrum. For de-convolution, a generic quadratic function is used as a survival probability;

Solar+KamLANDsin2θ12=0.308 Δm2

21=7.50x10-5eV2

Solarsin2θ12=0.311 Δm2

21=4.85x10-5eV2

SK recoil electron spectrum constrain the fit parameters (ci) of the function and the allowed Pee(En) is derived using the allowed (ci).

f8B=5.25 x 106/(cm2∙sec)

fhep=7.88 x 103/(cm2∙sec)

Page 31: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Multiple scattering goodness

Induced multiple scattering goodness(MSG) in SK-IV analysis.

Although the 214Bi decay-electrons (majority of low energy BG) fluctuate up above 5.0MeV, they truly have energy less than 3.3MeV and should have more multiple scattering than true 5.0MeV electrons.

3.5-4.0MeV

4.0-4.5MeV

MSG < 0.35

MSG < 0.35

MSG > 0.45

MSG > 0.45

35

Page 32: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

MSG

32

For each PMT hit pair, the vectors to the Chrenkov ring cross points are the direction candidates

MSG = vector sum of the candidates/ scalar sum of the candidates

MSG of multiple scattering events should be small

Page 33: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Comparison with others

BOREXINO

SNO KamLAND

Super-K

Super-K spectrum is the most precise!

33

Page 34: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Solar Neutrinos

SK & SNO

BORE-XINO

Cl

all solar BOREXINOBORE-XINO

8B

pp

Hep

pep

Pee

7Be

MSW (solar&KL)MSW (solar)

p+p d+e➝ ++νe

(99.77%)p+e-+p d+➝ νe

(0.23%)

3He+p α+e➝ ++νe

d+p➝3He+γ

3Ηe+α➝7Be+γ 15.08%

7Be+p➝8B+γ 0.1%

8B+➝8Be*+e++νe

3Ηe+3Ηe α+2p➝ 84.92%

7Li+p α+α;➝ 8Be* α+α➝

7Be+e-➝7Li+νe 99.9%

Page 35: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Super-K water transparency

35

anti-correlated with Supply water temperature

@ Cherenkov light wavelengthMeasured by decay e-e+ from cosmic m-m+

SK-IVSK-III

Started automatic temperature control

Page 36: Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain Solar Neutrinos in Super-Kamiokande ICHEP2014 @Valencia July 4 2014 1 Hiroyuki Sekiya ICRR, University

Hiroyuki Sekiya ICHEP2014 Jul. 4 2014 @Valencia, Spain

Convection suppression in SK

Very precisely temperature-controlled (±0.01oC) water is supplied to the bottom.

36

3.5MeV-4.5MeVEvent distributionReturn to

Water system

PurifiedWater supply

r2

Temperature gradation in Z

The difference is only 0.2 oC