Kam LAND Future Prospects Atsuto Suzuki Tohoku University

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Kam. LAND Future Prospects Atsuto Suzuki Tohoku University Kam. LAND Collaboration III Int. Workshop

Kam. LAND Future Prospects Atsuto Suzuki Tohoku University Kam. LAND Collaboration III Int. Workshop on Neutrino Oscillations in Venice Feb. 7 -10, 2006

Outline 1. Kam. LAND-II 2. Prospects of Solar Neutrino Detection 3. 3. Toward Precise

Outline 1. Kam. LAND-II 2. Prospects of Solar Neutrino Detection 3. 3. Toward Precise Measurement of 4. Reactor Neutrinos 5. 4. More and more Geoneutrinos 5. Conclusions

1. Kam. LAND-II (summer in 2006) ※ 7 Be solar neutrino detection: JSPS 5

1. Kam. LAND-II (summer in 2006) ※ 7 Be solar neutrino detection: JSPS 5 -year project from 2004 ※ Precise measurements of reactor-, geo- and solar neutrinos: MEXT 5 -year project from 2005 300 180 km Kam. LAND-II

2. Prospects of Solar Neutrino Detection single events in Kam. LAND 10 -5 ~

2. Prospects of Solar Neutrino Detection single events in Kam. LAND 10 -5 ~ 10 -6

distillation test bench Test Bench Studies 212 Pb 222 Rn R~10 -2 222 Rn

distillation test bench Test Bench Studies 212 Pb 222 Rn R~10 -2 222 Rn : 4 x 10 -3 >R > 5 x 10 -4 85 Kr : 4 x 10 -5 >R > 5 x 10 -6 N 2 purge test bench

Background Reduction Status impurities 238 U present (3. 5 ± 0. 5) x 10

Background Reduction Status impurities 238 U present (3. 5 ± 0. 5) x 10 -18 g/g 232 Th (5. 2 ± 0. 8) x 10 -17 g/g 40 K < 2. 7 x 10 -16 g/g 85 Kr ~ 1 Bq/m 3 210 Pb ~ 10 -20 g/g goal reduction 10 -16 g/g 10 -18 g/g ~1 m. Bq/m 3 ~10 -25 g/g OK OK 10 -2 10 -6 10 -5 distillation purge < 10 -2 < 10 -5 < 10 -4 < 10 -5 purification system installation : until this July space for new purification system (May 2005)

Expected Energy Spectrum in Kam. LAND-II 100 days data 210 Po 85 Kr events

Expected Energy Spectrum in Kam. LAND-II 100 days data 210 Po 85 Kr events (0. 3 <E< 0. 8 Me. V) / day / fid. (R< 4 m) 7 Be (80) , CNO (16), pep (4) , 85 Kr (8), 210 Bi (<2), 210 Po (<1), 40 K (3)

Seasonal Flux Variation of Solar Neutrinos 3 years data in Kam. LAND-II events (0.

Seasonal Flux Variation of Solar Neutrinos 3 years data in Kam. LAND-II events (0. 3 <E< 0. 8 Me. V)/ day / fid. (R < 4 m) 7 Be (80) , CNO (16), pep (4) , 85 Kr (8), 210 Bi (<2), 210 Po (<1), 40 K (3)

Possibility to Detect CNO and pep Neutrinos CNO+pep

Possibility to Detect CNO and pep Neutrinos CNO+pep

11 C Identification DL < 50 cm along m : # of neutrons >

11 C Identification DL < 50 cm along m : # of neutrons > 0 11 C with DR < 150 cm Present Kam. LAND Data Dt (DR : distance from the nearest n) 100 200 (min. ) energy 1. 2 1. 4 1. 6 1. 8 (Me. V) DR 200 400 600 800 (cm)

New Electronics for Identifying Successive Multiple Events new (dead-time free)

New Electronics for Identifying Successive Multiple Events new (dead-time free)

Expected Energy Spectrum in CNO+pep Region 90% rejection of 11 C 3 years data

Expected Energy Spectrum in CNO+pep Region 90% rejection of 11 C 3 years data 7 Be pep CNO 11 C

background subtracted 7 Be neutron tagging efficiency ~ 100% 3 years data CNO pep

background subtracted 7 Be neutron tagging efficiency ~ 100% 3 years data CNO pep

3. Toward Precise Measurement of Reactor Neutrinos ( ne nx : 2 -flavor case

3. Toward Precise Measurement of Reactor Neutrinos ( ne nx : 2 -flavor case ) shape-analysis Nobs – NBG Nexpected LMA II: disfavored at 98. 0% CL LAM I = 0. 686 ± 0. 044 (stat) ± 0. 045 (syst) disappearance: 99. 995 % CL LAM 0: disfavored at 97. 5% CL

Improvement of Detector Systematic Error energy scale, timing, g detection, n capture time, n

Improvement of Detector Systematic Error energy scale, timing, g detection, n capture time, n detection, trigger efficiency, light transport, …. 6. 5 % 4 % total uncertainty g n 12 N, 12 B, … m radioactive sources, laser system, LEDs, cosmic-ray m, m –induced spallation products : 1. 012 Me. V (g +System g) Off-Axis Calibration 65 68 Ge Zn : 1. 116 Me. V (g) 60 Co : 2. 506 Me. V (g + g) Am. Be : 2. 20 , 4. 40, 7. 6 Me. V (g)

Setting Off-Axis System

Setting Off-Axis System

Updated Oscillation Parameters statistics x 5 systematic error : 4% statistics x 5 statistics

Updated Oscillation Parameters statistics x 5 systematic error : 4% statistics x 5 statistics x 10 systematic error : 4% statistics x 10 limit due to 4% systematic error

4. More and More Geoneutrinos ne ne ne G. Gamow: 1953 ne ne

4. More and More Geoneutrinos ne ne ne G. Gamow: 1953 ne ne

Geoneutrino Result in Kam. LAND Background Kam. LAND Accidental Coincidence Events/0. 17 Me. V

Geoneutrino Result in Kam. LAND Background Kam. LAND Accidental Coincidence Events/0. 17 Me. V 13 C (a, n) 16 O Reactor ne short lived long lived Th U Antineutrino Energy (Me. V) Total signal # of events 2. 38 ± 0. 01 42 ± 11 best fit 80. 4 ± 7. 2 1. 9 ± 0. 2 127 ± 13 152

Constraints on FU +FTh & FU /FTh in Kam. LAND-II Th/U~3. 9 NU +

Constraints on FU +FTh & FU /FTh in Kam. LAND-II Th/U~3. 9 NU + NTh CL 68. 3% CL 95. 4% CL 99. 7% BSE model best fit (NU – NTh)/(NU + NTh) 2 years data in Kam. LAND-II

2 years data in Kam. LAND-II Th/U~3. 9

2 years data in Kam. LAND-II Th/U~3. 9

Conclusions Kam. LAND-II provides • high rate detection of 7 Be solar neutrinos, •

Conclusions Kam. LAND-II provides • high rate detection of 7 Be solar neutrinos, • chance to detect CNO + pep solar neutrinos, • stringent constraint on Dm 2 for reactor neutrinos, • more constraint on U+Th (geoneutrinos), and • interesting test of U/Th (geoneutrinos)