15,900 research outputs found

    Recent Results from the K2K (KEK-to-Kamioka) Neutrino Oscillation Experiment

    Get PDF
    The latest results of the K2K experiment are reported. The results are based on data taken from June, 1999, to June, 2000, corresponding to a total 2.610192.6 \cdot 10^{19} protons on target. Twenty seven fully-contained events in the 22.5 kton fiducial volume of Super-Kamiokande (SK) are observed. The expected number of events is estimated to be 40.3^{+4.7}_{-4.6} assuming the null oscillations hypothesis.Comment: 7 pages, 7 figures. Talk given at the Sixth International Workshop on Tau Lepton Physics, Victoria, BC, Canada, September 19, 200

    Solar Neutrino Oscillation Parameters after KamLAND

    Full text link
    We explore the impact of the data from the KamLAND experiment in constraining neutrino mass and mixing angles involved in solar neutrino oscillations. In particular we discuss the precision with which we can determine the the mass squared difference Δmsolar2\Delta m^2_{solar} and the mixing angle θsolar\theta_{solar} from combined solar and KamLAND data. We show that the precision with which \Delta m^_{solar} can be determined improves drastically with the KamLAND data but the sensitivity of KamLAND to the mixing angle is not as good. We study the effect of enhanced statistics in KamLAND as well as reduced systematics in improving the precision. We also show the effect of the SNO salt data in improving the precision. Finally we discuss how a dedicated reactor experiment with a baseline of 70 km can improve the θsolar\theta_{solar} sensitivity by a large amount.Comment: Talk given at 4th International Conference on Nonaccelerator New Physics (NANP 03), Dubna, Russia, 23-28 Jun 200

    Four species neutrino oscillations at ν\nu-Factory: sensitivity and CP-violation

    Get PDF
    The prospects of measuring the leptonic angles and CP-odd phases at a {\em neutrino factory} are discussed in the scenario of three active plus one sterile neutrino. We consider the \nu_\mu \raw \nu_e LSND signal. Its associated large mass difference leads to observable neutrino oscillations at short (1\sim 1 km) baseline experiments. Sensitivities to the leptonic angles down to 10310^{-3} can be easily achieved with a 1 Ton detector. Longer baseline experiments (100\sim 100 km) with a 1 Kton detector can provide very clean tests of CP-violation especially through tau lepton detection.Comment: 15 pages, LaTeX2e, 14 eps files, use package epsfi

    Super-Kamiokande data and atmospheric neutrino decay

    Get PDF
    Neutrino decay has been proposed as a possible solution to the atmospheric neutrino anomaly, in the light of the recent data from the Super-Kamiokande experiment. We investigate this hypothesis by means of a quantitative analysis of the zenith angle distributions of neutrino events in Super-Kamiokande, including the latest (45 kTy) data. We find that the neutrino decay hypothesis fails to reproduce the observed distributions of muons.Comment: 6 pages (RevTeX) + 2 figures (Postscript

    A new parametrization of the neutrino mixing matrix for neutrino oscillations

    Get PDF
    In this paper we study three active neutrino oscillations, favored by recent data from SuperK and SNO, using a new parametrization of the lepton mixing matrix VV constructed from a linear combination of the unit matrix II, and a hermitian unitary matrix UU, that is, V=cosθI+isinθUV = \cos\theta I + i\sin \theta U. There are only three real parameters in VV including the parameter θ\theta. It is interesting to find that experimental data on atmospheric neutrino dictates the angle θ\theta to be π/4\pi/4 such that the νμ\nu_\mu and ντ\nu_\tau mixing is maximal. The solar neutrino problem is solved via the MSW effect with a small mixing angle, with UU depending on one small parameter ϵ\epsilon. The resulting mixing matrix with just two parameters (θ\theta and ϵ\epsilon) predicts that the oscillating probabilities for νeνμ\nu_e\to \nu_\mu and νeντ\nu_e \to \nu_\tau to be equal and of the order 2ϵ2=(0.252.5)×1032\epsilon^2 = (0.25\sim 2.5)\times 10^{-3}. The measurement of CP asymmetries at the proposed Neutrino Factories would also provide a test of our parametrization.Comment: 10 pages, Retex, no figure

    Weak and Electromagnetic Nuclear Decay Signatures for Neutrino Reactions in SuperKamiokande

    Full text link
    We suggest the study of events in the SuperKamiokande neutrino data due to charged- and neutral-current neutrino reactions followed by weak and/or electromagnetic decays of struck nuclei and fragments thereof. This study could improve the prospects of obtaining evidence for τ\tau production from νμντ\nu_\mu \to \nu_\tau oscillations and could augment the data sample used to disfavor νμνsterile\nu_\mu \to \nu_{sterile} oscillations.Comment: 7 pages, latex, to appear in Phys. Rev. Let

    Searching for νμντ\nu_\mu \to \nu_\tau Oscillations with Extragalactic Neutrinos

    Full text link
    We propose a novel approach for studying νμντ\nu_\mu \to \nu_\tau oscillations with extragalactic neutrinos. Active Galactic Nuclei and Gamma Ray Bursts are believed to be sources of ultrahigh energy muon neutrinos. With distances of 100 Mpc or more, they provide an unusually long baseline for possible detection of νμντ\nu_\mu \to \nu_\tau with mixing parameters Δm2\Delta m^2 down to 101710^{-17}eV2^2, many orders of magnitude below the current accelerator experiments. By solving the coupled transport equations, we show that high-energy ντ\nu_\tau's, as they propagate through the earth, cascade down in energy, producing the enhancement of the incoming ντ\nu_\tau flux in the low energy region, in contrast to the high-energy νμ\nu_\mu's, which get absorbed. For an AGN quasar model we find the ντ\nu_\tau flux to be a factor of 2 to 2.5 larger than the incoming flux in the energy range between 10210^2 GeV and 10410^4 GeV, while for a GRB fireball model, the enhancement is 10%-27% in the same energy range and for zero nadir angle. This enhancement decreases with larger nadir angle, thus providing a novel way to search for ντ\nu_\tau appearance by measuring the angular dependence of the muons. To illustrate how the cascade effect and the ντ\nu_\tau final flux depend on the steepness of the incoming ντ\nu_\tau, we show the energy and angular distributions for several generic cases of the incoming tau neutrino flux, Fν0EnF_\nu^0 \sim E^{-n} for n=1,2 and 3.6. We show that for the incoming flux that is not too steep, the signal for the appearance of high-energy ντ\nu_\tau is the enhanced production of lower energy μ\mu and their distinctive angular dependence, due to the contribution from the τ\tau decay into μ\mu just below the detector.Comment: 11 pages, including 4 color figure
    corecore