The Main Injector Neutrino Oscillation Search (MINOS) experiment uses an acceleratorproduced neutrino beam to perform precision measurements of the neutrino oscillation parameters in the "atmospheric neutrino" sector associated with muon neutrino disappearance. This long-baseline experiment measures neutrino interactions in Fermilab's NuMI neutrino beam with a near detector at Fermilab and again 735 km downstream with a far detector in the Soudan Underground Laboratory in northern Minnesota. The two detectors are magnetized steel-scintillator tracking calorimeters. They are designed to be as similar as possible in order to ensure that differences in detector response have minimal impact on the comparisons of event rates, energy spectra and topologies that are essential to MINOS measurements of oscillation parameters. The design, construction, calibration and performance of the far and near detectors are described in this paper.
This Letter reports new results from the MINOS experiment based on a two-year exposure to muon neutrinos from the Fermilab NuMI beam. Our data are consistent with quantum-mechanical oscillations of neutrino flavor with mass splitting |Deltam2| = (2.43+/-0.13) x 10(-3) eV2 (68% C.L.) and mixing angle sin2(2theta) > 0.90 (90% C.L.). Our data disfavor two alternative explanations for the disappearance of neutrinos in flight: namely, neutrino decays into lighter particles and quantum decoherence of neutrinos, at the 3.7 and 5.7 standard-deviation levels, respectively.
This paper describes the hardware and operations of the Neutrinos at the Main Injector (NuMI) beam at Fermilab. It elaborates on the design considerations for the beam as a whole and for individual elements. The most important design details of individual components are described. Beam monitoring systems and procedures, including the tuning and alignment of the beam and NuMI longterm performance, are also discussed.
The velocity of a ∼3 GeV neutrino beam is measured by comparing detection times at the Near and Far detectors of the MINOS experiment, separated by 734 km. A total of 473 Far Detector neutrino events was used to measure (v − c)/c = 5.1 ± 2.9 × 10 −5 (at 68% C.L.). By correlating the measured energies of 258 charged-current neutrino events to their arrival times at the Far Detector, a limit is imposed on the neutrino mass of mν < 50 MeV/c 2 (99% C.L.).
A search for depletion of the combined flux of active neutrino species over a
735 km baseline is reported using neutral-current interaction data recorded by
the MINOS detectors in the NuMI neutrino beam. Such a depletion is not expected
according to conventional interpretations of neutrino oscillation data
involving the three known neutrino flavors. A depletion would be a signature of
oscillations or decay to postulated non-interacting "sterile" neutrinos,
scenarios not ruled out by existing data. From an exposure of 3.18x10^{20}
protons on target in which neutrinos of energies between ~500 MeV and 120 GeV
are produced predominantly as nu_mu, the visible energy spectrum of candidate
neutral-current reactions in the MINOS far detector is reconstructed.
Comparison of this spectrum to that inferred from a similarly selected near
detector sample shows that of the portion of the nu_mu flux observed to
disappear in charged-current interaction data, the fraction that could be
converting to a sterile state is less than 52% at 90% confidence level (C.L.).
The hypothesis that active neutrinos mix with a single sterile neutrino via
oscillations is tested by fitting the data to various models. In the particular
four-neutrino models considered, the mixing angles theta_{24} and theta_{34}
are constrained to be less than 11 degrees and 56 degrees at 90% C.L.,
respectively. The possibility that active neutrinos may decay to sterile
neutrinos is also investigated. Pure neutrino decay without oscillations is
ruled out at 5.4 standard deviations. For the scenario in which active
neutrinos decay into sterile states concurrently with neutrino oscillations, a
lower limit is established for the neutrino decay lifetime tau_3/m_3 >
2.1x10^{-12} s/eV at 90% C.L..Comment: 18 pages, 17 figures. Published in Phys. Rev.
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