MINERvA Overview MINERvA is studying neutrino interactions in unprecedented detail on a variety of different nuclei Low Energy (LE) Beam Goals: – Study.

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Presentation transcript:

MINERvA Overview MINERvA is studying neutrino interactions in unprecedented detail on a variety of different nuclei Low Energy (LE) Beam Goals: – Study both signal and background reactions relevant to oscillation experiments (current and future) – Measure nuclear effects on exclusive final states as function of a measured neutrino energy Study differences between neutrinos and anti-neutrinos – Precise understanding important for oscillation expt’s Medium Energy (ME) Beam (NOvA) Goals: – Structure Functions on various nuclei – Study high energy feed-down backgrounds to LBNE NuMI Beamline Provides – High intensity, Wide range of available energies MINERvA detector Provides – Reconstruction in different nuclei, broad range of final states Low Energy and Special Run Fluxes ~100 Particle, Nuclear, and Theoretical physicists from 22 Institutions

MINERvA Detector Basics Nuclear Targets – Allows side by side comparisons between different nuclei – Solid C, Fe, Pb, He, water Solid scintillator tracker – Tracking, particle ID, calorimetric energy measurements – Low visible energy thresholds Side and downstream Electromagnetic and Hadronic Calorimetry – Allow for event energy containment MINOS Near Detector – Provides muon charge and momentum ECALECAL HCALHCAL Nuclear Targets cryogenic target

MINERvA Data One out of three views shown, color=energy Single Electron candidate Quasi-elastic candidate Deep Inelastic Scatter candidate Resonant candidate

MINER A: Quasi-Elastic Analysis 4 Relatively Simple Final state – Require Muon, plus little or no extra energy Primary interaction type for neutrino oscillation experiments Measuring muon energy and angle (with respect to the beam) reconstructs a quasi- elastic interaction: –neutrino energy –momentum transfer to nucleon (Q 2 ) Preliminary analysis of first half of anti- neutrino data taken during final detector construction period, represents about 1/10 of current data set. –Statistical errors only Anti-neutrino, 0.4 ×10 20 POT, partial detector (~10% of data) Anti-neutrino, 0.4 ×10 20 POT, partial detector (~10% of data) First shown at NuINT’11, Dehradun India

MINER A: Special Runs to understand Neutrino Flux 5 Goal: to test flux model by taking neutrino data in several different configurations – Map through pion production spectrum – Change transverse and longitudinal focusing – Standard candle cross sections should be independent of incident neutrino flux Capability unique to NuMI beamline Standard candles available: – Inclusive Charged Current events – Quasi-Elastic Events Have taken 4 special run configurations – Medium, High energy target positions – Horn off data (no focusing) Developing Data Reconstruction and Flux Tuning Infrastructure in parallel Reconstructed neutrino energy of charged current candidates in standard running and three neutrino mode special runs Reconstructed neutrino energy of charged current candidates in special run in antineutrino mode and 0 horn current

MINER A: Nuclear Target Analysis 6 MINERvA has 5 solid nuclear targets – Different thicknesses good for different analyses: most downstream target best for exclusive final state analyses First look at inclusive Charged Current (CC) events from Fe and Pb TargetFiducial Mass  CC Events in 4×10 20 POT Plastic6.43 tons1363k Helium0.25 tons56k Carbon0.17 tons36k Water0.39 tons81k Iron0.97 tons215k Lead0.98 tons228k Neutrino Mode 1.3×10 20 POT Target 5 only (1/15 of expected sample) First shown at NuINT’11, Dehradun India