E - GDR neutrino
Transcription
E - GDR neutrino
Etat d’avancement du projet OPERA/CNGS D.Duchesneau LAPP, Annecy • Introduction • CNGS beam-line • OPERA experiment: – status of construction – Physics performance • Conclusion Réunion du GDR ν CPPM, 14 mars 2005 CNGS/OPERA program: In the CERN high energy νµ beam (CNGS): • search for ντ appearance at the Gran Sasso laboratory (732 km from CERN) Answer unambiguously on the origin of the ν oscillations observed at the atmospheric ∆m2 scale • search for νµ → νe and put new constraints on θ13 Most recent atmospheric results: Super-Kamiokande : (hep-ex/0501064): SK L/E analysis : PRL 93 (2004) 101801: Best fit: ∆m2 = 2.1 10-3 eV-2 and sin22θ = 1.0 1.5 < ∆m2 < 3.4 x 10-3 eV2 at 90% CL Best fit: ∆m2 = 2.4 10-3 eV-2 and sin22θ = 1.0 1.9 < ∆m2 < 3.0 x 10-3 eV2 at 90% CL CNGS: beam optimized for ντ appearance For 1 year of CNGS operation in shared mode: “Off-peak”: 200 days/year ; ε = 55% 4.5 x 1019 pot/year νµ CC / kton 2900 νµ NC / kton 875 < E >ν ( GeV ) 17 (νe + νe) / νµ 0.85 % νµ / νµ 2.1 % ντ prompt negligible OPERA: ~ 30 evts/day For ∆m2=2.4x10-3 and maximal mixing expect 16 ντ CC/kton/year at Gran Sasso Status of the project: Civil engineering is completed (June 2003) Hadron stopper and decay tube installed (June 2004) Installation of the services going on until June 2005 Hadron stop: Sept. 2003 Target chamber: June 2003 Decay tube: 998 m vacuum tested April 2004 Proton beam and target chamber installation: second semester 2005 Inner Conductor of the Horn Inner Conductor of the Reflector June 2003 at LAL with the Outer Conductor Delivered to CERN Feb. 2005 April 2004 at CERN Work to complete by CERN First beam to Gran Sasso in spring 2006 Gran Sasso National Laboratory: ( Italy, 120 km from Rome) Underground laboratory: 1400 m good cosmic ray shielding 1 cosmic/m2/hr 3 large experimental halls (100m x 18m x 18m) directed towards CERN Hall B ICARUS Borexino HallC OPERA Belgium IIHE(ULB-VUB) Brussels Bulgaria Sofia University COLLABORATION China IHEP Beijing, Shandong Croatia Zagreb University France July 2000: Experiment proposal May 2003 Start construction Summer 2006 First beam expected LAPP Annecy, IPNL Lyon, LAL Orsay, IRES Strasbourg Germany Berlin, Hagen, Hamburg, Münster, Rostock Israel Technion Haifa Italy Bari, Bologna, LNF Frascati, L’Aquila, LNGS, Naples, Padova, Rome, Salerno Japan Aichi, Toho, Kobe, Nagoya, Utsunomiya Russia INR Moscow, ITEP Moscow, JINR Dubna, Obninsk 36 groups ~ 165 physicists Switzerland Bern, Neuchâtel Turkey METU Ankara Newcomer in 2005: Tunis group γ . cτ < 1 mm ντ π, e, µ Experimental signature for ντ appearance: τ νe νµ ντ p,n,π,K... τ decay modes: µ- ν τ ν µ h- ντ nπο e- ντ νe π+ π- π- ντ nπο ΒR 17.4 % 49.5 % 17.8 % 15.2 % detect and identify the ντ CC events OPERA: direct observation of τ decay topology ¾ See the τ decay kink or multiprong topology at sub-millimetre distance of the ν interaction vertex requires nuclear emulsions: ~ µm granularity needs large target mass: Emulsion Cloud Chamber technique ¾ Reject efficiently main topological background: charm production prompt µ at primary vertex wrong sign assignment at secondary vertex pt imbalance criteria 250 evts/year OPERA: CERN experiment CNGS1 direct ντ observation by DONUT in 2000 use photographic emulsions alternate emulsion films with lead sheets (ECC concept) plastic base 200 µm thick Modular detector: basic unit brick 1 mm ν 8cm 12.5cm 10X0 56 Pb sheets (1mm) 57 FUJI emulsion films 1 changeable sheet τ ν Pb emulsion layers (50 µm thick) 206 336 bricks are needed → target mass: 1.8 ktons 1.8 kton detector at Gran Sasso (Hall C) µ spectrometer: Dipolar magnet + RPC chambers Precision tracker: Drift tubes B=1.6 T ν brick (56 Pb/Em. “cells”) Target Trackers Pb/Em. target • 2 SuperModules • 31 walls/SuperModule • 52x64 bricks/wall • 206 336 bricks module brick wall scintillator strips 8 cm (10X0) Status of construction Technical layout in Hall C 1st SM 2nd SM ~ 10 m ~20 m ~ 10 m Muon spectrometer Fe Total Fe weight ~ 1 kton RPC 22 planes of 21 chambers 2.9 m x 1.1m copper strips 6 planes of drift tubes B= 1.55 T (5 cm) Bakelite RPC: Precision tracker 8.2 m 12 Fe slabs in total coil •Tube : vertical , φ = 38 slabs base •efficiency: 99.1% installation started: may 2003 miss ≈ ( 0 . 1÷0 . 3 )% ε charge ∆p/p < 20% for p<50 GeV mm, length 8 m , wire φ = 50 µm • Plane: 4 staggered layers, each with 168 tubes • resolution: < 300 µm µId > 95% (with Target Tracker) Hall C in Gran Sasso: July 2003 Assembly frame for vertical slabs OPERA magnet assembly coil Antiseismic structure Base magnet 2 Magnet Assembly in Hall C september 2003 June 2004 • Magnet SM1 completed June 2004 • Magnet SM2 partially assembled, should be completed in April 2005 Drift tube module RPC: 1160 chambers produced + all needed strips for the 2 SM •Mechanical test, gas tightness •HV, electrical tests in Ar •Noise, Efficiency with cosmics Gas and HV tests repeated in Hall C Precision tracker: full size prototype (Hamburg) Mass production started in January 2005 Installation: 48 modules in April 2005 and 48 modules in August 2005 8m Target tracker: • Plastic scintillator strips: 6.7 m x 2.5 cm x 1 cm •AMCRYS-H (Kharkov) readout by Kuraray WLS optical fibres + Hamamatsu PMT 64 channels • X and Y planes of 256 strips ν •Target Tracker tasks : - trigger (ε > 99%) - brick finding: εbrick = 70-80% - initiate muon tagging Module assembly in Strasbourg (IRES) Target tracker production: • 235 modules already produced (~50%) • 220 modules already calibrated, • 832 PMTs delivered (80%) Mounting and storing in Hall C (Aug 2004) Commissioning of the electronics (FE chips LAL) and DAQ (IPNL) at LNGS in progress •Mechanical Structure Extended, completed for SM1 August 2004 • Target Section SM1 startedSept 2004 OPERA Hall C : september 04 Target walls: mass production going on. Rate: 2 half-walls/week December 04: first brick wall installed in Hall C • Installation procedure needs optimisation • Target installation paused • Some modifications in support structure foreseen • Target Installation should resume beginning of May 2005 The Bricks: Germany Japan 100mm LEAD 12 million plates 125mm Emulsion films 12 million sheets Italy In Gran Sasso underground area: automatic Piling and packaging 2 bricks/mn → 1 year production Fuji Emulsion Films • Mass production started April 2003 (~150 000 m2) • Already 50% produced. To be completed in autumn 2005 • Refreshing done in the Tono Mine in Japan to erase cosmic ray tracks before transportation o 30 C, 95% RH 3 days • batch sent to LNGS every 2 months starting January 2005 •Already 2.2 million refreshed Fuji films received and stored in Gran Sasso (~20%) Lead Low radioactivity lead (Boliden) Pb +2.5 % Sb •Thickness control: 1000 µm +− 10µm) (~107 plates to be produced for OPERA) Brick Assembly Machine (BAM) Hall A Lead from Boliden Hall B • Construction started in Tecno-Cut firm • BAM site in preparation at Gran Sasso • Aug-Sept 2005: Delivery and assembly at Gran Sasso • Dec 2005-Dec 2006: Brick mass production: 1000 /day Brick Manipulators (LAPP): • Full test in Annecy in 2005 • Installation in Gran Sasso in autumn • Start filling the walls Dec 2005 Annecy, January 2005 Automatic Scanning: Nagoya and Europe R&D efforts S-UTS prototype at Nagoya European station Bari, Bern, Bologna, Lyon, Napoli, Neuchatel, Roma, Salerno 500 fps CMOS camera Dedicated hardware Hard coded algorithms Commercial hardware Software algorithms 15 microscopes working Scanning speed ~ 20 cm2/h/side Single side microtrack finding efficiency ~ 95% • Fast CCD camera (3 k frames/sec) • Continuous movement of the X-Y stage Sheet-to-sheet alignment (8 GeV/c πs) ~ 0.5 µm Angular resolution ~ 2 mrad νµ → ντ search Exploited τ decay channels τ → e “ long decays ” τ → µ “ long decays ” τ → h “ long decays ” kink angle θkink > 20 mrad ε.BR = 2.8-3.5% τ→ e “ short decays ” τ → µ “ short decays ” impact parameter I.P. > 5 to 20 µm ε.BR = 0.7-1% Expected number of background events after 5 years: τ→e Charm background .210 τ→µ .010 τ→h .162 total .382 Large angle µ scattering .116 Hadronic background .093 .116 .209 .219 .278 0.707 Total per channel .210 .116 νµ → ντ search full mixing, 5 years run @ 4.5x1019 pot / year ¾New Brick finding strategy: eff. gain +10% ¾ Including the τ → 3 prongs (ε.BR = 1.0%): eff. gain +10% channel e µ h 3h total Signal (∆m2 (eV2)) 1.9 10-3 2.4 10-3 3.0 10-3 2.7 4.3 6.7 2.2 3.6 5.6 2.4 3.8 5.9 0.7 1.1 1.7 8.0 12.8 19.9 ε.BR Background 3.7% 3.1% 3.3% 1.0% 11.1% 0.23 0.23 0.32 0.22 1.00 Improvements under study ¾ Reduction of the number of background events (~30%): improve π/µ id. (low p) using dE/dx vs range: reduce the charm background New measurement of the large angle µ scattering New estimates of the hadronic background using Chorus data 4σ discovery potential and sensitivity versus Beam Intensity Opera with beam upgrade and 30% 90 % CL Sensitivity F&C BCK reduction Opera, with beam upgrade (1.5) Opera nominal (but with 3pi and new BF ) SK 90% CL (L/E analysis) Opera with 30% bck reduction νµ → νe search: Assuming ∆m122 << ∆m232 = ∆m132 = ∆m2, in the 3 flavour ν oscillation framework P(νµ -> ντ)= cos4θ13 sin22θ23 sin2(1.27 ∆m2 L/E) subleading transition P(νµ -> νe)= sin2θ23 sin22θ13 sin2(1.27 ∆m2 L/E) •look for an excess of νe CC events νe beam νµ → νe ν µ → ντ Events Both oscillations distort Evis at low energy Events •take into account electron event from νµ → ντ , τ → eντνe NC νe beam νµ → νe ν µ → ντ NC Fit oscillation components simultaneously sin22θ13 Visible Energy (GeV) use Evis, PTmiss, Eel sin22θ13 Missing pT (GeV) νµ → νe expected signal and background 5 years: 2.25x1020 pot θ13 sin2 2θ13 Signal νµ−>ντ , νµ CC νµ NC νe CC (deg) νµ−>νe τ −> eντνe 9 0.095 9.3 4.5 1.0 5.2 18 7 0.058 5.8 4.6 1.0 5.2 18 5 0.030 3.0 4.6 1.0 5.2 18 ∆m223 (eV2) OPERA sensitivity to θ13 Preliminary 4.50 1019 pot/yr 6.76 1019 pot/yr sin22θ13 syst. on the νe contamination up to 10% Limits at 90% CL for ∆m2 = 2.5x10-3 eV2 full mixing CHOOZ OPERA sin2 2θ13 <0.14 <0.06 θ13 110 7.10 Conclusions CNGS beam: on schedule → expect to start in June 2006 OPERA: construction and installation is progressing → should be ready to record ν events in 2006 Physics with CNGS: νµ → ν τ : • first evidence for ντ appearance signal after a few years • expect 13 τ events after 5 years with 1.0 background event at ∆m2 ~ 2.4 10-3 eV2 • studies to improve efficiency and to reduce background are going on νµ → ν e : • high detector capabilities to explore this channel • θ13 limit down to 70 • sensistivity on θ13 with a dependence on δCP different from T2K The End