The NOvA Experiment Ji Liu On behalf of the NOvA collaboration College of William and Mary APS April Meeting April 1, 2012.

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Presentation transcript:

The NOvA Experiment Ji Liu On behalf of the NOvA collaboration College of William and Mary APS April Meeting April 1, 2012

NOvA APS April Meeting -- Ji Liu2  Long-baseline neutrino oscillation experiment currently under construction  Off-axis neutrinos from NuMI beam  Two identical mostly active liquid scintillator detectors  Near Detector: serves as a non-oscillation reference  Far Detector: measure oscillations  Primary goal: observe and study and  oscillations at the atmospheric oscillation length/energy.  Gives NOvA sensitivity to θ 13, mass hierarchy, δ cp  Secondary goal: measure sin 2 θ 23 and Δm 2 32 to better precision

Neutrino Oscillation Channels APS April Meeting -- Ji Liu3  Accelerator experiments looks for ν e appearance  Oscillation probability depends on sin 2 2θ 13, sin 2 θ 23, δ cp and mass hierarchy  Probability can differ between and Δm 2 sol Δm 2 atm Δm 2 sol Δm 2 atm Normal Hierarchy Inverted Hierarchy

Detectors APS April Meeting -- Ji Liu4  Massive, 65% active Far Detector  15 kton, 810 km from source  Functionally equivalent Near Detector  220 ton, 1 km from source  Both have fine spatial resolution to distinguish ν e and NC events  0.15 X 0 per layer 63m PVC extrusion + Liquid Scintillator Read out via WLS fiber to APD

MC Events in NOvA APS April Meeting -- Ji Liu5 Beam μ p+p+ e Small shower from 2 nd γ Reject 995/1000 background events and achieve 26% efficiency

Off-Axis Feature APS April Meeting -- Ji Liu6 Both detectors will be sited 14 mrad off the NuMI beam axis.  Increase low-energy neutrino flux  Narrow energy spectra enhances background rejection  narrow band beam peaked at 2 GeV, well matched to peak oscillation probability

Sensitivity to Mass Hierarchy APS April Meeting -- Ji Liu7 Normal Hierarchy Inverted Hierarchy Daya Bay results Daya Bay results is assuming 2sin 2 (θ 23 ) = 1

Far Detector Construction APS April Meeting -- Ji Liu8 First block in place ~ early June 2012 First block filled ~ Aug 2012 First block outfitted ~ Nov 2012

Near Detector On the Surface (NDOS) APS April Meeting -- Ji Liu9  Near detector prototype constructed on the surface in Fall 2010  Currently taking data from the NuMI & Booster neutrino beams  Physics goal of NDOS:  Study response of the detector to neutrinos  Investigate the cosmic ray background  Calibrate the detectors (Seen T. Kutnink’s talk for more details) Top View Side View

Michel Electrons APS April Meeting -- Ji Liu  Use for electro-magnetic energy calibration  Easy to identify by looking at the end of the muon tracks for late hits  Have average ~ 4 hits per event 10 Here colors of the cells represent time, green hits are 4 μs later than blue ones Michel e PRELIMINARY

Conclusion APS April Meeting -- Ji Liu11  NOvA is on track to make many important contributions to neutrino physics  Measurement of θ 13  Determination of mass hierarchy  More precise measurements of Δ m 2, sin 2 (2 θ 23 )  Far detector construction is starting and will take its first data in ~ 1 year  Prototype detector has been running for one year  Studying calibration  Initial studies of neutrino interactions

Back-up Slides APS April Meeting -- Ji Liu12

Neutrinos Oscillation Channels APS April Meeting -- Ji Liu13  ν e disappearance reactor experiments  Looking for ν e disappearance  Probability depends on sin 2 2θ 13 and Δm 2  CHOOZ, Double-Chooz and Daya Bay L/E (km/MeV) Solar L/E Atmospheric L/E P( ν e -> ν e )

Neutrinos APS April Meeting -- Ji Liu14  Neutrinos have two sets of eigenstates  Weak eigenstates (ν e, ν μ, ν τ )  Mass eigenstates (ν 1, ν 2, ν 3 )  Neutrinos oscillations come about because the weak eigenstates are rotated from the mass eigenstates. weak eigenstatesmass eigenstates unitary mixing matrix

Neutrinos: What we know APS April Meeting -- Ji Liu15  Mixing angle:  Mass Hierarchy Mu-> tao E -> mu, tao Mu -> e Atmospheric neutrinos: Solar neutrinos: Sin2(2θ13) = ± 0.016(stat) ± 0.005(syst) Reactor + Solar, L/E~15 km/MeV atmospheric and accelerator, L/E~0.5 km/MeV

Neutrinos: What we don’t know APS April Meeting -- Ji Liu16  Mass Hierarchy  CP violation phase is unconstrained Neutrino mass hierarchy Individual mass of neutrino Delta m atm 2 Delta m sol 2

NOvA Features APS April Meeting -- Ji Liu17  Long baseline & Matter effects The neutrinos in the NuMI beam propagate through the earth and a coherent charged-current forward scattering of mu-e with electrons in the earth induces a significant change in the oscillation probabilities. These matter effects have opposite sign for neutrino and anti-neutrino and for the normal versus inverted neutrino mass ordering.  Optimized for the detection of both ν μ → ν e and ν μ → ν e oscillations NOvA will split its running time equally between neutrino running and antineutrino running. It will make the sensitivity to seeing a signal less dependent on the value of δ cp and the sign of Δm 2 and give NOvA the capability of measuring them.

Sensitivity to Mass Hierarchy Combing T2K Results APS April Meeting -- Ji Liu18 Normal Hierarchy Inverted Hierarchy Daya Bay results Daya Bay results is assuming 2sin 2 (θ 23 ) = 1