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Recent results of the OPERA experiment

Recent results of the OPERA experiment. Fabio Pupilli ( INFN – Laboratori Nazionali del Gran Sasso) on behalf of the OPERA Collaboration 26/09/2013 – XIV ICATPP – Villa Olmo, Como. Outline. Opera Collaboration 140 physicists , 28 institutions from 11 countries.

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Recent results of the OPERA experiment

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  1. Recent results of the OPERA experiment Fabio Pupilli (INFN – Laboratori Nazionali del Gran Sasso) on behalfof the OPERA Collaboration 26/09/2013 – XIV ICATPP – Villa Olmo, Como

  2. Outline Opera Collaboration 140 physicists, 28 institutionsfrom 11 countries • The OPERA experiment • Physics goal • Detector description • Detector operation • Status of data analysis • νµ  ντoscillationsearch status • νµ  νeoscillationsearch status Nihon Fabio Pupilli - XIV ICATPP

  3. OSCILLATION PROJECT WITH EMULSION TRACKING APPARATUS Goal: first direct observation of ντ appearance from νµ oscillation at atmospheric scale • Long Baseline (730 km) experiment in the CNGS (CERN Neutrino to Gran Sasso) νµ beam • Located in LNGS  1400 m rock overburden, low cosmic µ flux (1/m2/h) Fabio Pupilli - XIV ICATPP Conventionalhighenergybeamoptimisedforντ CC interactionsobservation Full coverage of the parameter space indicated by Super-K, K2K, MINOS Low νecontamination Constraints on νµνe oscillations *Interaction rate at LNGS

  4. - nm n The ntDetection principle The challenge istodistinguishντinteractionsfromνµinteractions, through the detection ofτleptonsproduced in ντ -CC interactions n Decay “kink” -, h-, 3h-, e- nm oscillation t- ct ~ 87 mm nt gct Eventbyeventtopological and kinematicalreconstruction Fabio Pupilli - XIV ICATPP ● Target mass O(kton) (low  interaction cross-section) ● High granularity detector ( decay detection, background rejection) lead – nuclear emulsion target segmented into basic units called bricks

  5. *JINST 4 (2009) P04018 The OPERA detector* SM1 SM2 Fabio Pupilli - XIV ICATPP Target area ~ 150000 ECC bricks  1.25 kton Muon Spectrometer Dipole Magnet + RPC + Drift Tubes Each brick followed by 2 removable emulsion films (CS) and planes of plastic scintillator strips in X/Y direction (TT) ECC (Emulsion Cloud Chamber) brick: 56 lead plates (1mm) + 57 emulsion films (300 µm)

  6. EVENT RECONSTRUCTION: ELECTRONIC DETECTORS* *[New J.Phys. 13 (2011) 053051] • Selectionofcontained and “on-time” events • Muonreconstructionand classificationasCC-like (1µ) or NC-like (0µ) • Muonmomentum and chargemeasurementthrough the spectrometer With µ: ・µ CC ・CC, τ→µ(17.7%) Develop this brick 20 m Without µ: ・µ NC ・CC, τ→e(17.8%) ・CC, τ→h,3h(64.5%) ・eCC Fabio Pupilli - XIV ICATPP • Identificationofinteractionbrick, using TT data in interplay with CS analysis

  7. nm_ Event Reconstruction: ECC Brick CSd • CS analysis: interface between electronic detectors(σpos~ 8 mm, σθ~ 15 mrad) and emulsion • CS tobrick connection (σpos~ 70 µm, σθ~ 8 mrad) and scan back: stoppingpointdefinition • Volume scan: topologicalvertexreconstruction and decaysearch 2 1 1 … 53 57 2 48 49 50 51 52 54 55 56 Fabio Pupilli - XIV ICATPP

  8. Event Reconstruction: Decay Search and Kinematical reconstruction • Decay topologies detected through: • kink angle along tracks attached to the vertex • Impact Parameter (IP) evaluation • IP distribution for: • - nt events (MC) • NC+CC nm events (MC) • NC+CC nmevents (Data) Fabio Pupilli - XIV ICATPP Momentum measurement Comparison with electronic detector (ED) measurement • Eventkinematicsreconstructedusing: • momentummeasurementby Multiple Coulomb Scatteringin lead[New J.Phys. 14 (2012) 013026] • e.m.showerenergymeasurementusingcalorimetrictechniques

  9. Status of Data Analysis *Proposal value: 22.5 x 1019 p.o.t. Fabio Pupilli - XIV ICATPP Target mass evolution -9.3% Target loss: ~ 112 tons Analysis still on going

  10. νµ ντCONTROL SAMPLE: CHARM EVENTS Charm lifetime and decaytopologiesanalogousto tau:  benchmark forτ decayfindingefficiency 2008  2010 data sample Expected events: 53 ± 5 Observed events: 50 Fabio Pupilli - XIV ICATPP Kolmogorov test ≥ 0.99

  11. The firstντ candidate Decay vertex: τ−→ρ− ντ ρ−→π0 π- π0 → γγ Fabio Pupilli - XIV ICATPP All primary tracks incompatible with muon hypothesis Found in 2008-2009 decaysearched data, released in 2010 [ Phys. Lett. B 691 (2010) 138 ]

  12. The secondντ candidate • Primary track incompatible with muon hypothesis • All tracks identified as hadrons • Event satisfies criteria for: • τ h+h-h-ντ [ arXiv:1308.2553 ] (submitted to JHEP) Fabio Pupilli - XIV ICATPP

  13. The thirdντ candidate Decay in plastic base Primary track incompatible with muon hypothesis Fabio Pupilli - XIV ICATPP Negative charge of the secondary muon assessed with 5.6 σ significance (by spectrometer measurement) Cuts for τ µchannel passed

  14. νµ  ντoscillationsearch status Preliminary *1µ 2011+2012 statisticsnotincluded Fabio Pupilli - XIV ICATPP *conservativenumber, assuming the whole 1µ 2011+2012 statistics 3 observedevents in the τ h , τ 3h , τ µ channels Combiningdifferentchannels, takinginto account differentsignaltonoiseratios: 3.4 σsignificanceofnon-nullobservation With a simple counting method  3.1 σ significance of non-null observation

  15. νµ  νeoscillationsearchstatus* * [ JHEP 1307 (2013) 004 ] 2008  2009 data sample 19 νe candidates observed 19.8±2.8 (syst.) events expected from bkg E = 15.6 GeV Fabio Pupilli - XIV ICATPP Three flavour mixing analysis (Ecut = 20 GeV): 4 observed events 4.6 expected Non standard oscillations at large Δm2 (Ecut = 30 GeV): 6 observed events 9.4 expected ⇒ sin2(2θ13) < 0.44 (90% C.L.) ⇒ sin2(2θnew) < 7.2 x 10-3 (90% C.L.)

  16. Conclusions • OPERA successfullyran on the CNGS neutrino beamfrom 2008 to 2012. Analysisisstill on going. • 17.97 x 1019p.o.t.werecollected (about 80% ofthe CNGS nominalvalue) • νµ ντoscillationresults: • Evidenceforνµ ντoscillation in appearance mode • 3 eventsobserved in the analysed sample • 3.4 σsignificanceofnon-nullobservation • More elaboratedstatisticalanalysis, exploitingkinematicalcharacteristicsof the events, under development • νµ νeoscillationresults: • Upper limitof 0.44 at 90% C.L. on sin2(2θ13) [threeflavour mixing] • Upper limitof 7.2 x 10-3 at 90% C.L. on sin2(2θnew) [non standard oscillations at largeΔm2] Fabio Pupilli - XIV ICATPP

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