DPG Spring Meeting Dresden 2013 Arnd Sörensen, Valentina Lozza, Nuno Barros, Belina von Krosigk, Laura Neumann, Johannes Petzoldt, Axel Boeltzig, Felix Krüger and Kai Zuber supported by: SNO+ = SNO + Liquid Scintillator ? Liquid Scintillator From SNO to SNO+ Phases of Operation Neodymium loaded Phase (0νββ with 150Nd) Pure Scintillator Phase SNO+ @ TU Dresden Summary & Outlook 2 @ SNOLab in Creighton Mine, Sudbury, Canada deepest underground laboratory 2 km ≈ 6000 meter water equivalent flat overburden muon rate: 3 acrylic vessel • 12 m diameter • 5 cm thickness 780 t liquid scintillator (LAB) ≈ 9100 PMTs in support structure (~ 54% coverage) light-water shielding: • 1700 t inside • 5700 t outside urylon liner and radon seal 4 LAB + PPO + (Nd) fluor: 2 g/L PPO (= 2,5-Diphenyloxazol) chemically compatible with acrylic long scattering length & high optical transparency high light yield (≈ 10,000 photons/MeV) high purity available inexpensive & safe 5 LAB lighter than water: SNO SNO+ rope hold up system + rope hold down system 6 General • rope-net hold down system • new calibration (source manipulation) system • scintillator purification plant 7 Electronics • DAQ boards refurbished • improved data flow • replace & repair broken PMTs • PMTs remapped 8 Calibration • new low energy sources • optical calibration via fibreinjected lasers and LEDs • variety of gamma, alpha, beta and neutron sources 9 2013 water phase 2014 2017/? (neutrinoless-) double beta decay 2017 ? pure scintillator • detector commissioning • 150Nd loaded into liquid scintillator • reactor-, geo- and supernova- neutrinos • search for solar neutrinos: pep and CNO • reactor-, geo- and supernova- neutrinos 10 neutrinoless 0vββ search • large isotope mass, low background • poor energy resolution with liquid scintillator 150Nd • high Q-value: 3.371 MeV low background • fastest calculated decay rate • complementary to other 0vββ experiments (76Ge, 136Xe …) in SNO+ • LS successfully loaded with Neodymium • 0.1% loading • optimisation: 0.3% loading 11 • 0.1% Nd loading (43.7 kg 150Nd) • mee = 350 meV • 6.4% FWHM @3.37 MeV • IBM‐2 matrix element • 3 years running and • 50% fiducial Volume (≈ 0.4 kt) • Borexino background levels + efficient tagging: 214Bi: 99.9% reduction 208Tl: 90.0% reduction Background despite low Q-value through pile-up of e.g. 144Nd, 176Lu, 138La, 14C 99% pile-up rejection while keeping 90% signal in ROI 12 Claim of Klapdor mee ≈ 170 – 530 meV 0.1% Nd (6.4% FWHM @ 3.37 MeV) [Nucl. Phys. B. (Proc. Supp.), S143:229, 2005] 0.3% Nd (9.0% FWHM @ 3.37 MeV) assuming Borexino background levels are reached and efficient tagging: 214Bi: 99.9% reduction 208Tl: 90.0% reduction 13 Complete our understanding of the solar neutrino fluxes: Super-K and SNO measured 8B neutrinos Borexino measured 7Be and first probed pep neutrinos pp was observed with Ga experiments improve pep measurement still missing CNO (probe for solar metallicity) 14 single energy: 1.442 MeV very well predicted flux (≈ 2% uncertainty) new physics models (NSI) predict different survival probabilities in vacuum matter transition regions [PLB 594, 347-354 (2004)] SNO, [arXiv:1109.0763] 15 old (high Z) new (low Z) [Peña-Garay & Serenelli, arXiv:0811.2424] No direct observation of CNO neutrinos yet ! probe for solar core metallicity new solar physics developments suggest 30% lower metallicity 16 no Oscillation 308 events no Oscillation 1186 events Oscillation 176 events Oscillation 710 events Flux is 5 times less than KamLAND BUT SNO+ reactor spectrum, including oscillations, have sharp peaks and minima, that increase the parameterfitting sensitivity for Δm12 17 Signal: n e + p ® e+ + n n e from β-decays in Earth’s mantle and continental crust (238U,232Th,40K) local region extremely well studied due to mining low reactor-v background in SNO+: Reactor/Geo ≈ 1.1 check Earth heat production models / chemical composition (multi-site measurement in combination with Borexino, KamLAND) 18 0vββ Phase • design, development and test of 48Sc calibration source (3.33 MeV - ROI) T 103.8 – Axel Boeltzig • study of cosmogenic (n,p)- activation of Nd and LAB • first measurement of natNd(p,x) cross sections [PRC 85, 014602 (2012)] • study of underground- and thermal- neutron activation of Nd pure scintillator phase • sensitivity study to solar neutrinos and neutrino oscillation parameters • design, development and test of 57Co low energy (122 keV) calibration source • to test the detector threshold and the low energy response • alpha and proton quenching factor measurements [arXiv:1301.6403] • cosmogenic muons and muon induced background tagging • investigation of the 14C background 19 SNO+ succeeds the SNO experiment by replacing heavy water with liquid scintillator LS has higher light yield and lower threshold allows to investigate lower energy range ( E < 3.5 MeV ) two phases planned: Nd loaded phase to search for 0vββ decay of 150Nd pure scintillator phase to observe pep and CNO solar neutrinos reactor neutrino oscillation confirmation, geo neutrino investigation at geologically-interesting site, supernova neutrino watch … SNO+ will be filled with water this year 0vββ search starts next year 20 Thank you for your attention ! 21 more 22 radio purity: 14C is not a problem pep signal is at higher energy U, Th not a problem if one can repeat KamLAND scintillator purity 40K, 210Bi (Radon daughter) 85Kr, 210Po not a problem pep signal is at higher energy Counts per 0.1 ktons per 1.0 years per 5 keV pep 11C pp pep be7 b8 cno c11-decays CNO Analytically generated spectra with 5%/ E resolution Borexino 104 103 102 11C 10 pep 1 1.2 1.4 1.6 1.8 2 visible energy [MeV] CNO 1 10-1 0 0.2 0.4 0.6 0.8 SNO + 23 p-p solar fusion chain CNO cycle 24 (stat) pep 8B 7Be pp CNO 1 year 2 years 9.1% 6.5% 7.5% 5.4% 4% 2.8% A few %? ~ 15%? Assuming Borexino-level backgrounds are reached Assuming Borexino-level backgrounds are reached