Underground Physics in the Pyhäsalmi mine

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Timo Enqvist University of Oulu, Finland Moscow, June 10, 2016 1/40

Content The Pyhäsalmi mine and Callio Lab Cosmic-ray experiment EMMA 14 C concentration in liquid scintillators Measurement of 2ν2β half-lives (β + EC mode) of 78 Kr and 124 Xe Moscow, June 10, 2016 2/40

The Pyhäsalmi Mine Moscow, June 10, 2016 3/40

The Pyhäsalmi mine Owned by First Quantum Minerals Ltd, Canada Active mine; procuding copper (Cu), zinc (Zn) and pyrite (FeS 2 ) The deepest metal mine in Europe 1400 m (4000 mwe) Very modern infrastructure lift (of 21.5 tons of ore or 20 persons) down to 1400 metres takes 3 minutes via 11-km long decline it takes 40 minutes (by track) good communication systems large caverns in good shape Underground mining operation is expected to end in 2019 Callio Lab Moscow, June 10, 2016 4/40

The Pyhäsalmi mine restaurant at 1410 m Moscow, June 10, 2016 5/40

The Pyhäsalmi mine maintenance hall at 1410 m Moscow, June 10, 2016 6/40

Callio Lab Underground mining operation in the Pyhäsalmi mine is expected to end in 2019 The mine has an excellent infrastructure, large caverns and halls, good location and possibility to excavate larger halls Callio Lab established to operate activities other than mining The first deep (1430 m, 4100 mwe) underground laboratory hall (120 m 2, 8 m height) ready for experiments C14 experiment neutron and muon background measurements ideal for small-scale experiments (dark matter, double-beta decay), for prototypes and testing, and for material screening Open Call to send a proposal (scientific or commercial) www.calliolab.com Moscow, June 10, 2016 7/40

Cosmic-ray experiment EMMA Moscow, June 10, 2016 8/40

EMMA the knee Moscow, June 10, 2016 9/40

EMMA muon lateral distribution cut-off energy 50 GeV (75 m of rock) Energy Composition CORSIKA + QGSJET 01 CORSIKA + EPOS 1.99 Moscow, June 10, 2016 10/40

EMMA detector geometry 75 m 45 m Moscow, June 10, 2016 11/40

EMMA detectors in tracking stations Moscow, June 10, 2016 12/40

EMMA detectors in sampling stations Moscow, June 10, 2016 13/40

EMMA DAQ running in 7 stations 75 m 45 m Moscow, June 10, 2016 14/40

Underground Physics in the Pyha salmi mine EMMA gas handling Total flux 8 `/min (Ar:CO2, 92:8) Moscow, June 10, 2016 15/40

Underground Physics in the Pyha salmi mine EMMA gas handling Total flux 8 `/min (Ar:CO2, 92:8) Moscow, June 10, 2016 16/40

Underground Physics in the Pyha salmi mine EMMA gas handling 94 m Total flux 8 `/min (Ar:CO2, 92:8) Moscow, June 10, 2016 17/40

EMMA stations C, F ja G Cavern properties ph 3 (water) rel. hum. 100 % T 10 C Moscow, June 10, 2016 18/40 Inside stations rel.hum. 40 60 % T 20 C Good conditions

EMMA drift chambers Former muon detectors from the DELPHI experiment at LEP (at CERN) a plank 7 individual chambers mass 120 kg per plank chamber: 365 cm 20 cm 3 signals per chamber In total 84 planks ( 250 m 2 ) form the basis of the array Position resolution is good: 1 cm 2 needed by tracking Ar (92%) : CO 2 (8%) at 1 bar min 0.25 bar l/min /4 planks Moscow, June 10, 2016 19/40

EMMA scintillation detectors SC16 detector 50 50 cm 2, H = 13 cm mass 20 kg per SC16 16 individual pixels of 12 12 cm 2 3 cm pixels APD light collection time resolution good: 1 ns Manufactured by Russian Academy of Sciences In total 96 SC16s (24 m 2, 1536 px), 72 SC16s in EMMA (1152 ps) Designed especially for large muon multiplisities fast trigger initial guest for the arrival angle Moscow, June 10, 2016 20/40

EMMA Limited Streamer Tube (LST) detectors Muon detectors of KASCADE Grande experiment (Karlsruhe) To be used as the second detector layer at the edge of the array and at 45-level Read-out electronics modified and is now being tested LSTs in operation by the end of 2016 60 LST modules 180 m 2 Properties 2.9 m 1.0 m pixel size (PAD): 2 cm 8 cm gas: CO 2 at 1 bar Moscow, June 10, 2016 21/40

EMMA first test runs with single stations (station C) Moscow, June 10, 2016 22/40

EMMA conclusions EMMA is an underground cosmic-ray experiment studing the knee region of the energy spectrum at the depth of 75 m = energy cut-off of 50 GeV It consists of 11 detector stations 7 stations currently in the DAQ, all stations by the end of 2016 three detector types: drift chambers, small-size plastic scintillation detectors and limited streamer tube detectors EMMA can extract the muon multiplicity, the lateral distribution and the arrival angle of an air shower angular accuracy 1 deg Simulations and data analysis packages under development first test runs (with multiplicities only) are looking fine Collaboration university of Oulu and university of Jyväskylä (Finland), Russian academy of sciences and Moscow institute of physics and technology (Russia), and university of Aarhus (Denmark) Moscow, June 10, 2016 23/40

C14 Experiment Measurement of 14 C/ 12 C ratio in liquid scintillator Moscow, June 10, 2016 24/40

C14 introduction 1 Measurement of 14 C/ 12 C ratio of several liquid scintillator samples Detector development currently the lowest concentration: 14 C/ 12 C 2 10 18 low-background liquid scintillator detector From the 14 C half life ( 5700 a) and the age of oil sources, the ratio 14 C/ 12 C should be 10 21 10 22 contamination from local environment (U, Th, K,...) Collaboration between university of Oulu, Finland university of Jyväskylä, Finland Russian Academy of Sciences, Russian Measurements in two laboratories Baksan Underground Laboratory, Russia, at 4900 mwe Pyhäsalmi Mine (CallioLab), Finland, at 4000 mwe similar method, similar shielding Moscow, June 10, 2016 25/40

C14 introduction 2 LAB (Linear Alkylbenzene) is currently the favoured liquid scintillator in large LS detectors SNO+ (1 kton) in Canada, JUNO (20 kton) in China 14 C concentration of LAB not measured before JUNO (Jiangmen Underground Neutrino Observatory) main scientific priority: neutrino mass hierarchy determination supernova neutrinos, solar neutrinos,... In JUNO the upper limit is: 14 C/ 12 C 10 17 The decay energy of 14 C is small (Q β =156 kev) usually below the threshold If the 14 C concentration too large = pulses may pile-up The 14 C concentration (of JUNO) to be measured in Baksan and Pyhäsalmi Moscow, June 10, 2016 26/40

C14 earlier measurements for 14 C/ 12 C 14 C/ 12 C ( 10 18 ) Liquid Scintillator Experiment [Ref] (1.94±0.09) PC+PPO Borexino CTF [1] (9.1±0.4) PXE+p-Tp+... Borexino CTF [2] (3.98±0.94) PC-Dodecane+PPO KamLAND [3] (12.6±0.4) PXE+p-Tp+... Dedicated setup [4] [1] G. Alimonti et al., Physics Letters B 422 (1998) 349 [2] H.O. Back et al., Nuclear Instrum. Methdos A 585 (2008) 48 [3] G. Keefer, arxiv:1102.3786 [4] C. Buck et al., Instrum. and Experim. Techniques 55 (2012) 34 Moscow, June 10, 2016 27/40

C14 14 C background in Borexino Borexino: 14 C/ 12 C 2 10 18 Moscow, June 10, 2016 28/40

C14 the instrument two low-background PMTs (ET 9302B, 3 ) quartz or acryllic vessel of 1.6 l (1350 g of LAB) acryllic light guides (20 30 cm long) VM2000 wrapping surrounded by thick layers (10 15 cm) of copper and lead liquid purified by Al 2 O 3 Moscow, June 10, 2016 29/40

C14 dedicated low-background hall in Baksan (4900 mwe) lead polyethylene cadmium Moscow, June 10, 2016 30/40

C14 the shielding at Baksan Copper 15 cm Moscow, June 10, 2016 31/40

C14 the laboratory hall at the Pyhäsalmi mine (Callio Lab 2) Moscow, June 10, 2016 32/40

C14 conclusions Only a few measurement of 14 C concentration in liquid scintillators exist the lowest measured concentration is 2 10 18 by Borexino CTF concentration of 14 C in Linear Alkylbenzene not previously measured Measurements started (in Baksan) and to be started (in Pyhäsalmi) for a series of 14 C concentration determination a dedicated setup 14 C concentration of the JUNO experiment will be determined An ultimate aim is to find a sample with a concentration of 10 20 low-backgound experiment Collaboration university of Oulu and university of Jyväskylä (Finland), Russian academy of sciences Moscow, June 10, 2016 33/40

Measurement of 2ν2β half lives of 78 Kr and 124 Xe (ECβ + mode) Moscow, June 10, 2016 34/40

2ν2β of 78 Kr and 124 Xe half-lives of 78 Kr Jouni Suhonen, Physical Review C 87 (2013) 034318, Analysis of double-β transitions in 78 Kr Moscow, June 10, 2016 35/40

2ν2β of 78 Kr and 124 Xe 2ν2β half-lives of 124 Xe Jouni Suhonen, Romanian Journal of Physics 58 (2013) 1232, Positron-emitting and double-ec modes of double beta decay Moscow, June 10, 2016 36/40

2ν2β of 78 Kr and 124 Xe previous measurements 78 Kr C. Sáenz et al., Phys. Rev. C 50 (1994) 1170, Results of a search for double positron and electron-positron conversion of 78 Kr Yu.M. Gavrilyuk et al., Phys. Atom. Nuclei (2000) 2201, New limit on the half-life of 78 Kr with respect to the 2K(2ν)-capture decay mode Yu.M. Gavrilyuk et al., Phys. Rev. C 87 (2013) 035501, Indications of 2ν2K capture in 78 Kr Yu.M. Gavrilyuk et al., Phys. Atom. Nuclei 76 (2013) 1063, Results of experiments devoted to searches for 2K capture on 78 Kr and for the double-beta decay of 136 Xe with the aid of proportional counters 124 Xe A.S. Barabash et al., Phys. Lett. B 223 (1989) 273, Results of the experiment on the search for double beta decay of 136 Xe, 134 Xe and 124 Xe Yu.M. Gavrilyuk et al., arxiv:1507.04520v1 [nucl-ex] 16 Jul 2015, Search for 2K(2ν)-capture of 124 Xe Moscow, June 10, 2016 37/40

2ν2β of 78 Kr and 124 Xe an idea for the experiment Liquid scintillator (LAB) of 500 1000 l (active volume) acryllic cylinder with PMTs at the ends gamma and neutron shielding by liquid scintillator or water of 20 tons 5% of enriched Kr and Xe mixed with the liquid the maximum amounts of mixing should be studied At the Pyhäsalmi mine (Callio Lab) at the depth of 1430 m (4100 mwe) Moscow, June 10, 2016 38/40

2ν2β of 78 Kr and 124 Xe conclusions An idea to measure 2ν2β half lives of the ECβ + mode of 78 Kr and 124 Xe with a liquid scintillator setup active volume 500 1000 l active shielding Theoretical calculations predict half lifes of 10 22 23 years possible with a small-scale experiment Important for understanding nuclear stucture and matrix elements Collaboration university of Oulu and university of Jyväskylä (Finland), Russian academy of sciences Moscow, June 10, 2016 39/40

Conclusions The mine provides excellent conditions for scientific work More activities (scientific and commercial) are looked for (Callio Lab concept) due to the mine closure in 2019 new deep laboratory ready Open Call (at www.calliolab.com) Physics studies going on EMMA and C14 running or under construction background measurements to be started (muon and neutron flux) an idea for measuring 2ν2β decay of 78 Kr and 124 Xe Russian institutes have been strongly participated in EMMA and C14 experiments Institute of Nuclear Research of the Russian academy of sciences Moscow Institute of Physics and Technology Moscow, June 10, 2016 40/40