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n Physics at UCL MINOS and NEMO-III. Ruben Saakyan UCL Sheffield Particle Physics seminar 12 November 2003. Motivation. Neutrino Mixing Observed !. From KamLAND, solar n and atmospheric n. VERY approximately. Neutrino MASS What do we want to know?. Relative mass scale ( n -osc)
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n Physics at UCLMINOS and NEMO-III Ruben Saakyan UCL Sheffield Particle Physics seminar 12 November 2003
Motivation Neutrino Mixing Observed ! From KamLAND, solar n and atmospheric n VERY approximately
Neutrino MASSWhat do we want to know? • Relative mass scale (n-osc) • Mass hierarchy (n-osc and bb) • Absolute mass scale (bb +3H b) mmin~ 0 - 0.01 eV mmin~ 0.03 - 0.06 eV Dirac or Majorana preferred by theorists (see-saw) ne n1 n2 n3 Ue12 Ue22 Ue32 Mixing Only from bb From n-osc
MINOS outline • MINOS basics • Construction status and schedule • Atmospheric n’s • Physics reach
Why ? • Confirm SuperK with controlled n beam (K2K is first here) • Demonstrate oscillatory behaviour • Make first ever precise (10%) measurement of oscillation parameters Dm232, sin2 2q23 • Improving existing result (CHOOZ) on subdominant nm ne (Ue3)
Who ? Main Injector Neutrino Oscillation Study 32 institutions 175 physicists
FarDet~5.4kT 735km NearDet ~1kT Where and How ? Two functionally identical magnetized steel/scintillator sandwich calorimeters
How ? (Part II) Expected event spectrum (from NearDet) Observed event spectrum (from FarDet) Ratio: survival probability as a Function of energy Shape: Oscillations? Decay? Other? Mixing angle Dm2
NuMI beam # protons on target 5 year plan nm CC events/8×1020 pot (~2.5 yr) Year 2005 2006 2007 2008 2009 Total Protons 2.5 3.8 5.0 6.5 7.2 25 ( × 1020) Lots of work to make it possible Low Medium High 5,080 13,800 29,600
677 m decay pipe Near Detector Target Construction @ Fermilab. The Beam Decay pipe is finished and encased in concrete Horns in fabrication Tunneling is finished • NuMI beamline completed Dec 2004 • Jan-Mar 2005 – Beam commissioning • Apr 2005 – Start of physics running October’03: Target Hall outfitting complete Beneficial occupancy of Near Detector hall – January 2004
Detector Technology • 1” thick steel planes • Extruded plastic scintillator strips • XY orientation of scint planes • WLS fiber + Hamamatsu multianode • PMTs: M16 (Far) and M64 (Near) • <B> = 1.5 Tl (Far and Near) • Front-ends • VA(IDE) – M16 • QIE – M64 • Software trigger
MINOS Far Detector • 8 m octagonal 1” steel plates • 2 Supermodules 15 m each • 5.4 kT total mass • 484/485 scintillator/steel planes • 2-ended readout • 8X optical multiplexing • ~1000 Km of scintillator • ~2000km of WLS + clear fiber • ~26000m2 of active detector planes • <B> ~ 1.5 Tl • DE/Ehadronic 55%/E • DE/Eem 22%/E • DP/Pm 12% (by curvature) • 6% (by range)
Far Detector at Soudan • Completed July 2003 • Magnetized and running • Half the detector has been running since mid 2002 • Fully commissioned • Taking atmospheric neutrino data, Soudan 2 exposure by the end of next year
Reconstructed front view Timing Cosmic ray muons • Cosmic ray muons are used for calibration (and physics!) • 2.6ns/plane timing resolution permits direction determination • Veto shield tags incoming “parallel” muons which can mimic neutrino events
Veto shield Atmospheric n’s at FarDetVeto Shield Veto shield to veto vertical muons and reduce background
Upward muons Downward • Timing allows measurement of 1/ • Good separation of downward (cosmic ray) and upward (neutrino induced) muons Upward
Atmospheric n events at FarDet 700 MeV muon • Atmospheric n interactions • have been observed • B-field allows to measure • muons up to 70 GeV • B-field gives charge info: • distinguish n and nbar • Potential to test CPT Num of events in 5 years nbar Contained vertex with m 620 400 Upgoing m 280 120
Near Detector n target • ~1 kT • High rates ~ 3 MHz • 3.8 x 4.8 “squeezed” octagon • 1-end readout • no-multiplexing • 220 M64sQIE-based front-end • 282 steel planes • 153 scintillator planes • Use events with R<30cm • EnNear EnFar • interactions in ND ~10 – 100 n events/spill • • ~108 – 109 events/yr • Unique opportunity • for n-scattering physics m spectrometer
Construction @ FermilabNear Detector • All NearDet planes assembled • and ready to install • Beneficial occupancy of • NearDet Hall – Jan 04 • Installation starts January 04 • Installation complete – Oct 04
Calibration Detectorat CERN • Both ND and FD too big to • be calibrated in test beam • CalDet is the same but smaller • T7 and T11 beamlines at CERN PS • in 2001, 2002, 2003 • October 2003: Data taking • programme complete • Understand detector response to • p, e, m, p of 0.5 – 10 GeV (particle ID) • Calibrate out Near/Far readout • differences • Debug detector subsystems • Refine topology and pattern recognition • software • 60 planes (1m×1m) 12 ton • 24 strips/plane, XY orientation in consecutive planes • FarDet and/or NearDet readout
Pion Proton Odd Plane view Even Plane view Even Plane view Odd Plane view Strip Strip Relative Pulse Height Relative Pulse Height 3.5 GeV 3.5 GeV Plane Plane 2 GeV 2 GeV 1 GeV 1 GeV Calibration Detector Events
MINOS:Physics Reach nmnt 2.3 yr* 3.7 yr* 5.0 yr* *Times according to 5 year proton intensity plan
MINOS:Physics Reach nmne
Summary • The MINOS Far Detector is complete and taking cosmic and atmospheric n data • Beam work and Near Detector construction at FNAL is on schedule. First beam – end 2004. • Calibration Detector programme at CERN complete • Physics running with NuMI n’s – April 2005
NEMO Outline • bb decay basics • The NEMO-III detector • First results • Sensitivity by 2008 • Towards NEMO-NEXT
bb decay basics Requires Majorana mn≠ 0 In many even-even nuclei b-decay is energetically forbidden SM Qbb This leaves bb as the allowed decay mode Qbb
bb Decay Basics. Rates G – phase space, exactly calculable; G0n ~ Qbb5, G2n ~ Qbb11 M – nuclear matrix element. Hard to calculate. Uncertainties factor of 2-10 (depending on isotope) Must investigate several different isotopes! <mn> is effective Majorana neutrino mass Isotopes of Interest 48Ca, 76Ge, 100Mo, 150Nd,136Xe, 116Cd, 96Zr, 82Se,130Te
Currently Active Experiments CUORICINO (bolometer) NEMO-3 (Tracking calorimeter) <mn> = 0.4 eV ??? Heidelberg-Moscow exp is still running ???
Neutrino Ettore Majorana Observatory 40 physicists and engineers 13 Laboratories/Universities 7 Countries
UK NEMO team (so far) • Phil Adamson, Leo Jenner, Ruben Saakyan, Jenny Thomas (all UCL) • Received approval from PPRP 27 Jan 03 • Main involvement: data analysis.. • ..and some hardware tasks: PMT helium tests, light injection optimization • Expect to participate in shifts at Frejus
From scintil detector: • st = 250 ps • From tracker: • s||= 1cm s = 0.45mm • (using timing information • on plasma propagation) • Calibration: • Laser survey • neutron Am/Be for • s||, s, e+ signature • e-207Bi, 90Sr for • energy calibration • 60Co for time alignment Trigger: 1 scintillator hit > 150 keV + 1 track: few Geiger planes (flexible 3 – 7 Hz)
NEMO bb events • 3D pictures • study single electron spectra • study angular distributions • Detailed 2n information • O (105) 2n100Mo events/yr ! • 7 isotopes
NEMO background events g e+e- e- (~7 MeV) from ng
Data taking • June 2002: start with all 20 sectors, iron shielding, neutron shielding but… • …still a lot of debugging (both tracking detector and calorimeter) • 14 February 2003: start of routine data taking
NEMO-3 First Results100Mo 1200 h 2n: T1/2=[7.4±0.05(stat)±0.8(sys)]×1018yr (19000 events; S/B 50) 0n: 1 event in 2.8 – 3.2 MeV region T1/2 > 1023 yr 90% CL <mn> < 0.9 – 2.1 eV World’s best result for 100Mo Very preliminary (and conservative) from 3800h: T1/2 > 2.3×1023 yr <mn> < 0.6 – 1.4 eV
Single State Dominance (SSD)VS Higher order State Dominance (HSD) Simkovic, Domin, Semenov nucl-th/0006084, Phys. Rev. C HSD 1+ 100Tc SSD 0+ 100Mo 0+ 100Ru • Shape of single e- spectrum • Shape of 2b spectrum • Angular distribution • ~ 20% difference in T1/2 100Mo + NEMO-like detector can test it experimentally !
NEMO-3 First Results100Mo 1200 h single e- spectrum Angular distribution between two e- Preliminary: SSD is preferred
NEMO-3 First Results Other Isotopes 116Cd 82Se 150Nd T1/2=[3.9±0.3(stat)±0.4(sys)]×1019 T1/2 > 1.0 × 1022 y 90% CL T1/2=[8.2±0.4(stat)±0.8(sys)]×1019 T1/2 > 4 × 1022 y 90% CL World’s best result ! T1/2=[7.0±0.7(stat)±0.7(sys)]×1018 T1/2 > 7.7 × 1020 y 90% CL
NEMO-3 0nbb sensitivity5 years E = 2.8 – 3.2 MeV 100Mo 7 kg Qbb =3.034 MeV External BG: 0 Internal BG: radioactivity < 0.04 event/y/kg 2nbb = 0.11 event/y/kg T1/2 > 3 × 1024 yr <m> < 0.2 – 0.5 eV 82Se 1 kg Qbb =2.995 MeV External BG: 0 Internal BG: radioactivity < 0.01 event/y/kg 2nbb = 0.01 event/y/kg T1/2 > 1 × 1024 yr <m> < 0.6 – 1.2 eV In case of full load of 82Se (~14kg) <m> < 0.1 – 0.3 eV
T1/2(2n) and Energy Resolution 82Se looks most promising candidate F ~ (sE/E)6
SuperNEMO ~ 100 kg 82Se (or other) • Sensitivity <mn> ~ 0.03 eV in 5 yr • Feasible if: • BG only from 2n • (NEMO3) • b) DE/E = 5-6% • at 3 MeV (Qbb82Se) • (R&D needed) 4 supermodules, planar geometry
Future bb projects comparison5yr exposure * 5 different latest NME calculations
Concluding Remarks • First (preliminary) results from NEMO-III: • <mn> ≤ 0.6 eV after 3800h • 2n: SSD is preferred • NEMO-III to reach 0.1 – 0.3 eV with 10 – 14 kg 82Se upgrade • UK involvement: 1000cm3 HP Ge detector • bb excited states physics with this Ge detector • Happy to collaborate with Sheffield and Boulby