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nEXO MATTHEW COON FOR THE EXO-200 COLLABORATION UNIVERSITY OF - PowerPoint PPT Presentation

Recent results of EXO- 200 and sensitivity of nEXO MATTHEW COON FOR THE EXO-200 COLLABORATION UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN DPF 2017, FERMILAB CHICAGO 1 ith 136 136 Xe: 0 wit 136 Xe 136 Ba ++ + 2e - , Q-value 2458 keV


  1. Recent results of EXO- 200 and sensitivity of nEXO MATTHEW COON FOR THE EXO-200 COLLABORATION UNIVERSITY OF ILLINOIS AT URBANA-CHAMPAIGN DPF 2017, FERMILAB CHICAGO 1

  2. ith 136 136 Xe: 0 νββ wit 136 Xe → 136 Ba ++ + 2e - , Q-value 2458 keV • Double Beta decay is the most sensitive probe for the Majorana nature of the neutrino. • Observation of the 0 νββ would provide: • A lepton number violating process for physics beyond the standard model. • Imply the Majorana nature of the neutrino. • Constrain the absolute mass scale of the neutrino. If neutrino is Majorana particle, decay can proceed without emitted neutrinos giving a peak at the Q-value. 2

  3. EX EXO-200 Detector: • Radiopure TPC filled with LXe enriched to 80.6% • Simultaneous measurements of both light and charge: • light collection with large avalanche photo-diode (APD) planes. • charge collection with 2 wire grids (induction and collection on each wire grid set). • HV is applied between the cathode in the middle of the TPC and anodes placed at each opposing end of the TPC. • Monolithic detector provides great background rejection capabilities. Full 3D reconstruction of events 3

  4. EX EXO-200 ope operatio ions: EXO-200 is located at the Waste Isolation Pilot Plant (WIPP) in Carlsbad, NM approx. 2,150 ft. underground. 4

  5. Detec ector up upgrades for Pha hase II II: • Front-end readout electronics replaced, • System to suppress radon from the air reducing APD readout noise. gap. (Not removing radon from LXe!) • HV raised by 50% from -8kV -> -12kV. • Direct air sampling shows radon reduction • Energy Resolution: by factor greater than 10. • Phase I: σ /E(Q) = 1.38% • Phase II: σ /E(Q) = 1.23% 5

  6. Detector Performance: De Position Discrimination: Using induction and collection wire grids, categorize single- Energy Resolution: site (SS) and multi-site (MS) events giving discrimination Use anticorrelation between between γ -like events and β -like events. scintillation and ionization energy. • SS fraction approx. 20% in energy ROI. • Calculate “standoff” Use rotated energy axis distance (SD) for each to optimize resolution event where β -like in the energy region of events should be more interest. evenly distributed throughout TPC. Use light/charge ratio to cut α’s from β / γ events 6

  7. De Detector Performance: Spatial distribution of standoff distance: • Calculate standoff distance of each event. • LXe self shielding provides independent measurement of γ backgrounds. • Looking at the distribution of standoff distances for each event, β events will be more uniformly distributed throughout the TPC. (additional discrimination between β / γ ) 7

  8. Fur Further disc discrim imin inatio ion be between γ’s and β’s: • Allow further γ -like rejection in SS events by looking at cluster size. (γ -source) 8

  9. Disc iscrim imin inators for or fi fit: • Combine SD, Number of collection channels, and Rise time into one variable using Boosted • Energy decision tree (BDT) machine learning. • SS/MS • BDT gives approx. 15% sensitivity improvement. • Standoff Distance BDT Discriminator • Number of • Final fit will be simultaneous channels ML with energy and BDT in SS. variable trained on SS events. • Signal rise times in SS. 9

  10. of 137 137 Xe: Neu eutron cap apture an and β -de decay of Muons entering the TPC can create neutron showers, yielding neutron capture via 136 Xe + n -> 137 Xe, which then β -decays. • Veto same half of the TPC as the γ for approx. 5 half-lives (19.1 min). • Can suppress 137 Xe β -decay using veto • Exposure loss approx. 3%. panel and de-excitation γ’s information. • Approx. 25% rejection, Phase-I: 7 -> 4.4 counts. 10

  11. Blin linded: • Blind analysis. • Background model + fit ML fit. • Combined phase-I and phase-II profiles. (Total exposure of 177.6 kg yr) Blinded energy ROI 11

  12. Un Un-bli linded: • Blind analysis. • Background model + fit ML fit. • Combined phase-I and phase-II profiles. (Total exposure of 177.6 kg yr) Un-blinded energy ROI • No statistical excess in energy ROI. • Combined p- value of approx. 1.5 σ . 12

  13. Res esult lts: • EXO-200 scheduled for another 1.5 year of • Results show no statistical excess of events in the data collecting. energy ROI with 177.6 kg yr exposure. • 0 νββ sensitivity improved by a factor of 2. • Continued data collection will improve the 0 νββ sensitivity. • Independent analysis of phase-I and phase-II. 13

  14. nEXO at nE t SNOLAB: • nEXO is a proposed 5000 kg (5 t) next generation LXe TPC. • EXO-200 has validated this approach showing good energy resolution with anticorrelation between scintillation light and ionization charge. • EXO-200 has demonstrated the power of large homogeneous detector giving promise to the detector performance goals of nEXO. • If tagging of the barium daughter nucleus from ββ -decay can be achieved, a virtually background free event measurement can be made. 14

  15. Base aseli line de desig ign for or nE nEXO: • Cold (in LXe) front end electronics. • Spherical carbon fiber cryostat (lighter than copper). • Charge readout pads (anode). • 4m 2 SiPM (high gain) staves e  lining the inside of the barrel. • Reflective cathode. 1.3m • Large single drift volume. (1.3m) Xe * Φ 1.3m 15

  16. nE nEXO pr proj ojected sen sensit itiv ivit ity an and di discovery ry po potentia ial: l: • Assumes baseline design of: • Existing materials (radiopure). • Energy resolution of 1%. (EXO-200 1.2%). • Improvement of SS/MS discrimination by factor of 2. 16

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  18. Univer ersi sity of Alabama, Tuscaloosa AL, USA Laurent entian n Univer ersi sity, Sudbury ON, Canada M Hughes, I Ostrovskiy, A Piepke, AK Soma, V Veeraraghavan B Cleveland, A Der Mesrobian-Kabakian, J Farine, A Robinson, U Wichoski Univer ersi sity of Bern, Switzerland — J-L Vuilleumier Lawrenc ence e Liver ermore e National Laboratory, Livermore CA, USA Brookhaven en National Laboratory, Upton NY, USA O Alford, J Brodsky, M Heffner, A House, S Sangiorgio M Chiu, G Giacomini, V Radeka, E Raguzin, T Rao, S Rescia, T Tsang Univer ersi sity of Massa ssachu huset etts, Amher herst st MA, USA Califo fornia Inst stitute e of Technology, Pasadena CA, USA — P Vogel S Feyzbakhsh, S Johnston, CM Lewis, A Pocar Carlet eton Univer ersi sity, Ottawa ON, Canada McGill Univer ersi sity, Montreal QC, Canada — T Brunner, Y Ito, K Murray I Badhrees, M Bowcock, W Cree, R Gornea, K Graham, T Koffas, C Licciardi, D Sinclair Oak Ridge e National Laboratory, Oak Ridge TN, USA — L Fabris, RJ Newby, K Ziock Colorado State e Univer ersi sity, Fort Collins CO, USA Pacifi fic Northwest est National Laboratory, Richland, WA, USA C Chambers, A Craycraft, W Fairbank Jr, D Harris, A Iverson, J Todd, T Walton I Arnquist, EW Hoppe, JL Orrell, G Ortega, C Overman, R Saldanha, R Tsang Drex exel el Univer ersi sity, Philadelphia PA, USA Renssel sselaer er Polytec echnic Inst stitute, Troy NY, USA — E Brown, K Odgers MJ Dolinski, E Hansen, YH Lin, E Smith, Y-R Yen Univer ersi sité é de Sher erbrooke — F Bourque, S Charlebois , M Côté, D Danovitch, Duke e Univer ersi sity, Durham NC, USA — PS Barbeau H Dautet, R Fontaine, F Nolet, S Parent, JF Pratte, T Rossignol, J Sylvestre, F Vachon Univer ersi sity of Erlangen en-Nurem ember erg, Erlangen en, Germany SLAC National Accel eler erator Laboratory, Menlo Park CA, USA G Anton, R Bayerlein, J Hoessl, P Hufschmidt, A Jamil, T Michel, M Wagenpfeil, T Ziegler J Dalmasson, T Daniels, S Delaquis, A Dragone, G Haller, LJ Kaufman, A Odian, M Oriunno, B Mong, PC Rowson, K Skarpaas IBS Center er for Under erground nd Physi sics, Daejeon, South Korea — DS Leonard Univer ersi sity of South Dakota, Vermillion SD, USA — J Daughhetee, R MacLellan IHEP Beijing, People ’ s Republic of China — G Cao, W Cen, Y Ding, X Jiang, Stanfo ford Univer ersi sity, Stanford CA, USA Z Ning, X Sun, T Tolba, W Wei, L Wen, W Wu, X Zhang, J Zhao R DeVoe, D Fudenberg, G Gratta, M Jewell, S Kravitz, G Li, A Schubert, M Weber, S Wui IME Beijing , People’s Republic of China — L Cao, X Jing, Q Wang Stony ny Brook Univer ersi sity, SUNY, Stony Brook NY, USA — K Kumar, O Njoya, M Tarka ITEP Mosc scow, Russia Technical Univer ersi sity of Munich, Garching, Germany — P Fierlinger, M Marino V Belov, A Burenkov, A Karelin, A Kobyakin, A Kuchenkov, V Stekhanov, O Zeldovich TRIUMF, Vancouver BC, Canada Univer ersi sity of Illinois, Urbana-Champaign IL, USA — D Beck, M Coon, S Li, L Yang J Dilling, P Gumplinger, R Krücken, Y Lan, F Retière, V Strickland Indiana Univer ersi sity, Bloomington IN, USA — JB Albert, S Daugherty, G Visser Yale e Univer ersi sity, New Haven CT, USA — Z Li, D Moore, Q Xia Univer ersi sity of Califo fornia, Irvine, Irvine CA, USA — M Moe The nEXO Collaboration

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