74 research outputs found

    Searching For A Nondiagonal Mass Varying Mechanism In The νμ-ντ System

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    We use atmospheric neutrino data and MINOS data to constrain the MaVaN (mass varying neutrinos) mechanism. The MaVaN model was largely studied in cosmology scenarios and comes from the coupling of the neutrinos with a neutral scalar depending on the local matter density. For atmospheric neutrinos, this new interaction affects the neutrino propagation inside the Earth, and as consequence, induces modifications in their oscillation pattern. To perform such test for a nonstandard oscillation mechanism with a nondiagonal neutrino coupling in the mass basis, we analyze the angular distribution of atmospheric neutrino events as seen by the Super-Kamiokande experiment for the events in the sub-GeV and multi-GeV range and muon neutrinos (antineutrinos) in the MINOS experiment. From the combined analysis of these two sets of data we obtain the best fit for Δm322=2.45×10-3 eV2, sin2(θ23)=0.42 and MaVaN parameter α32=0.28 with modest improvement, Δχ2=1.8, over the standard oscillation scenario. The combination of MINOS data and Super-Kamiokande data prefers small values of MaVaN parameter α32<0.31 at 90% C. L. © 2014 American Physical Society.901ICTP; Abdus Salam International Centre for Theoretical PhysicsTauber, J., (2013) Astron. Astrophys., , (Planck Collaboration), doi: 10.1051/0004-6361/201321529. AAEJAF 0004-6361Jae, A., (2013) Astron. Astrophys., , (Planck Collaboration), doi: 10.1051/0004-6361/201321546. AAEJAF 0004-6361Tegmark, M., Eisenstein, D.J., Strauss, M.A., Weinberg, D.H., Blanton, M.R., Frieman, J.A., Fukugita, M., York, D.G., Cosmological constraints from the SDSS luminous red galaxies (2006) Physical Review D - Particles, Fields, Gravitation and Cosmology, 74 (12), p. 123507. , http://oai.aps.org/oai?verb=GetRecord&Identifier=oai:aps.org: PhysRevD.74.123507&metadataPrefix=oai_apsmeta_2, DOI 10.1103/PhysRevD.74.123507Riess, A.G., Filippenko, A.V., Challis, P., Clocchiatti, A., Diercks, A., Garnavich, P.M., Gilliland, R.L., Kirshner, R.P., Observational Evidence from Supernovae for an Accelerating Universe and a Cosmological Constant (1998) Astronomical Journal, 116 (3), pp. 1009-1038. , DOI 10.1086/300499Perlmutter, S., (1999) Astrophys. J., 517, p. 565. , (Supernova Cosmology Project Collaboration),. ASJOAB 0004-637X 10.1086/307221Astier, P., Guy, J., Regnault, N., Pain, R., Aubourg, E., Balam, D., Basa, S., Walton, N., The supernova legacy survey: Measurement of ΩM, ΩΛand w from the first year data set (2006) Astronomy and Astrophysics, 447 (1), pp. 31-48. , DOI 10.1051/0004-6361:20054185Einstein, A., (1917) Sitzungsber. Preuss. Akad. Wiss. Berlin (Math. Phys.), 1917, p. 142Weinberg, S., (1989) Rev. Mod. Phys., 61, p. 1. , RMPHAT 0034-6861 10.1103/RevModPhys.61.1Dolgov, A.D., (2004) Proceedings of 18th les Rencontres de Physique de la Vallee d'Aoste, 34. , in, Frascati Physics Series, edited by M. Greco (INFN, Frascati, Rome), Vol.Fardon, R., Nelson, A.E., Weiner, N., J. Cosmol. Astropart. Phys., 2004 (10), p. 005. , JCAPBP 1475-7516 10.1088/1475-7516/2004/10/005Kaplan, D.B., Nelson, A.E., Weiner, N., (2004) Phys. Rev. Lett., 93, p. 091801. , PRLTAO 0031-9007 10.1103/PhysRevLett.93.091801Gu, P., Wang, X., Zhang, X., Dark energy and neutrino mass limits from baryogenesis (2003) Physical Review D, 68 (8), p. 087301. , DOI 10.1103/PhysRevD.68.087301Bi, X.-J., Gu, P., Wang, X., Zhang, X., Thermal leptogenesis in a model with mass varying neutrinos (2004) Physical Review D, 69 (11), p. 113007. , DOI 10.1103/PhysRevD.69.113007Afshordi, N., Zaldarriaga, M., Kohri, K., (2005) Phys. Rev. D, 72, p. 065024. , PRVDAQ 1550-7998 10.1103/PhysRevD.72.065024Honda, M., Takahashi, R., Tanimoto, M., J. High Energy Phys., 2006 (1), p. 042. , JHEPFG 1029-8479 10.1088/1126-6708/2006/01/042Barger, V., Huber, P., Marfatia, D., Solar mass-varying neutrino oscillations (2005) Physical Review Letters, 95 (21), pp. 1-4. , http://oai.aps.org/oai/?verb=ListRecords&metadataPrefix= oai_apsmeta_2&set=journal:PRL:95, DOI 10.1103/PhysRevLett.95.211802, 211802Cirelli, M., Gonzalez-Garcia, M.C., Pena-Garay, C., Mass varying neutrinos in the Sun (2005) Nuclear Physics B, 719 (1-2), pp. 219-233. , DOI 10.1016/j.nuclphysb.2005.04.034, PII S0550321305003299Gonzalez-Garcia, M.C., De Holanda, P.C., Zukanovich Funchal, R., (2006) Phys. Rev. D, 73, p. 033008. , PRVDAQ 1550-7998 10.1103/PhysRevD.73.033008De Holanda, P.C., J. Cosmol. Astropart. Phys., 2009 (7), p. 024. , JCAPBP 1475-7516 10.1088/1475-7516/2009/07/024Rossi-Torres, F., Guzzo, M.M., De Holanda, P.C., Peres, O.L.G., (2011) Phys. Rev. D, 84, p. 053010. , PRVDAQ 1550-7998 10.1103/PhysRevD.84.053010Carneiro, M.F., De Holanda, P.C., (2013) Adv. High Energy Phys., 2013, p. 293425. , 1687-7357 10.1155/2013/293425Shiraishi, K.K., (2006), http://www-sk.icrr.u-tokyo.ac.jp/doc/sk/pub/, Ph.D. thesis, University of WashingtonAbe, K., (2008) Phys. Rev. D, 77, p. 052001. , (Super-Kamiokande Collaboration),. PRVDAQ 1550-7998 10.1103/PhysRevD.77. 052001Adamson, P., (2013) Phys. Rev. Lett., 110, p. 251801. , (MINOS Collaboration),. PRLTAO 0031-9007 10.1103/PhysRevLett.110.251801Adamson, P., (2011) Phys. Rev. Lett., 106, p. 181801. , (MINOS Collaboration),. PRLTAO 0031-9007 10.1103/PhysRevLett.106.181801In the MaVaN mechanism, neutrino and antineutrinos have the same oscillation probabilityGratieri, D.R., (2012), http://webbif.ifi.unicamp.br/tesesOnline/teses/IF1564.pdf, Ph.D. thesis, State University at Campinas (UNICAMP)Dziewonski, A.D., Anderson, D.L., (1981) Phys. Earth Planet. Inter., 25, p. 297. , PEPIAM 0031-9201 10.1016/0031-9201(81)90046-7For a good reference on kinematical constraints, see [30]Goldanski, V.I., Rosenthal, I.L., (1961) Kinematics of Nuclear Reactions, , (Oxford University Press, New York)Honda, M., Kajita, T., Kasahara, K., Midorikawa, S., Sanuki, T., (2007) Phys. Rev. D, 75, p. 043006. , PRVDAQ 1550-7998 10.1103/PhysRevD.75.043006Gonzalez-Garcia, M.C., Nunokawa, H., Peres, O.L.G., Stanev, T., Valle, J.W.F., (1998) Phys. Rev. D, 58, p. 033004. , PRVDAQ 0556-2821 10.1103/PhysRevD.58.033004Strumia, A., Vissani, F., (2003) Phys. Lett. B, 564, p. 42. , PYLBAJ 0370-2693 10.1016/S0370-2693(03)00616-6Paschos, E.A., Yu, J.Y., Neutrino interactions in oscillation experiments (2002) Physical Review D, 65 (3), p. 033002. , DOI 10.1103/PhysRevD.65.033002Hosaka, J., Ishihara, K., Kameda, J., Koshio, Y., Minamino, A., Mitsuda, C., Miura, M., Saji, C., Three flavor neutrino oscillation analysis of atmospheric neutrinos in Super-Kamiokande (2006) Physical Review D - Particles, Fields, Gravitation and Cosmology, 74 (3), p. 032002. , http://oai.aps.org/oai?verb=GetRecord&Identifier=oai:aps.org: PhysRevD.74.032002&metadataPrefix=oai_apsmeta_2, DOI 10.1103/PhysRevD.74.032002http://www-numi.fnal.gov/PublicInfo/forscientists.html, The (Equation presented) is avaliable inGonzalez-Garcia, M.C., Maltoni, M., Salvado, J., Schwetz, T., J. High Energy Phys., 2012 (12), p. 123. , JHEPFG 1029-8479 10.1007/JHEP12(2012)12

    Angra Neutrino Project: status and plans

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    We present the status and plans of the Angra Project, a new nuclear reactor neutrino oscillation experiment, proposed to be built in Brazil at the Angra dos Reis nuclear reactor complex. This experiment is aimed to measure theta_13, the last unknown of the three neutrino mixing angles. Combining a high luminosity design, very low background from cosmic rays and careful control of systematic errors at the 1% level, we propose a high sensitivity multi-detector experiment, able to reach a sensitivity to antineutrino disappearance down to sin^2(2*theta_13) = 0.006 in a three years running period, improving present limits constrained by the CHOOZ experiment by more than an order of magnitude.Comment: 2 pages, 1 figure, talk presented by J.C. Anjos ([email protected]) at NuFact05, 21-26 June 2005, Frascati, Ital

    Update On Atmospheric Neutrinos

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    We discuss the impact of recent experimental results on the determination of atmospheric neutrino oscillation parameters. We use all published results on atmospheric neutrinos, including the preliminary large statistics data of Super-Kamiokande. We reanalyze the data in terms of both vμ → vτ and vμ → ve channels using new improved calculations of the atmospheric neutrino flux. We compare the sensitivity attained in atmospheric neutrino experiments with those of accelerator and reactor neutrino oscillation searches, including the recent CHOOZ experiment. We briefly comment on the implications of atmospheric neutrino data in relation to future searches for neutrino oscillations with long baselines, such as the K2K, MINOS, ICARUS, and NOE experiments.5833300413300413Gaisser, T.K., (1997) Proceedings of the 17th International Conference on Neutrino Physics and Astrophysics, p. 211. , Neutrino '96, Helsinki, Finland, edited by K. Enquist, K. Huitu, and J. 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A, 363, p. 604. , http://www.na.infn.it/SubNucl/accel/noe/noe.htmlhttp://www.aquila.infn.it/icarus/Cavanna, F., (1995) A First 600 Ton ICARUS Detector Installed at the Gran Sasso Laboratory, , addendum to Proposal by the ICARUS Collaboration, Report No. LNGS-95/1

    Atmospheric neutrino data : Active-Active ×\times Active-Sterile oscillations

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    I summarize here the results of a global fit to the full data set corresponding to 33.0 kt-yr of data of the Super-Kamiokande experiment as well as to all other experiments in order to compare the active-active and active-sterile neutrinos oscillation channels to the atmospheric neutrino anomaly.Comment: 3 pages, uses espcrc2.sty (Nuclear Physics style) and epsfig.sty, 2 PS files. To appear in the Proceedings of the XTH Int. Symposium on Very High Energy Cosmic Ray Interactions, Laboratory Nazionali del Gran Sasso, Assergi, Italy, July 12-17 199

    Effects of non-standard neutrino interactions on MSW-LMA solution to the solar neutrino problem

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    We show that the non-standard neutrino interactions can play a role as sub-leading effect on the solar neutrino oscillations. We observe that very small flavor universality violations of order of 0.1-0.2 G_F is sufficient to induce two phenomena: suppression of the eletronic neutrino earth regeneration and a shift of the resonance layer in the sun. We obtain these phenomena even in the absence of any flavor changing interactions. We discuss their consequences and confront with a global analysis of solar+KamLAND results. We conclude that a new compatibility region in the Delta m^2 x tan^2\theta, which we call very low Large Mixing Angle region, is found for Delta m^2 ~ 1e-5 eV^2 and tan^2\theta= 0.45.Comment: references added, small changes in text, some changes in predictions of KamLAND future sensitivity to NSNI parameter

    Sum Rules of Neutrino Masses and CP Violation in the Four-Neutrino Mixing Scheme

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    We show that the commutator of lepton mass matrices is invariant under terrestial matter effects in the four-neutrino mixing scheme. A set of model-independent sum rules for neutrino masses, which may be generalized to hold for an arbitrary number of neutrino families, are for the first time uncovered. Useful sum rules for the rephasing-invariant measures of leptonic CP violation have also been found. Finally we present a generic formula of T-violating asymmetries and expect it to be applicable to the future long-baseline neutrino oscillation experiments.Comment: RevTex 8 pages. 3 references added. Phys. Rev. D (in printing

    Status of atmospheric neutrino(mu)<-->neutrino(tau) oscillations and decoherence after the first K2K spectral data

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    We review the status of nu_mu-->nu_tau flavor transitions of atmospheric neutrinos in the 92 kton-year data sample collected in the first phase of the Super-Kamiokande (SK) experiment, in combination with the recent spectral data from the KEK-to-Kamioka (K2K) accelerator experiment (including 29 single-ring muon events). We consider a theoretical framework which embeds flavor oscillations plus hypothetical decoherence effects, and where both standard oscillations and pure decoherence represent limiting cases. It is found that standard oscillations provide the best description of the SK+K2K data, and that the associated mass-mixing parameters are determined at 1 sigma (and d.o.f.=1) as: Delta m^2=(2.6 +- 0.4)x10^{-3} eV^2 and sin^2(2theta)=1.00+0.00-0.05. As compared with standard oscillations, the case of pure decoherence is disfavored, although it cannot be ruled out yet. In the general case, additional decoherence effects in the nu_mu-->nu_tau channel do not improve the fit to the SK and K2K data, and upper bounds can be placed on the associated decoherence parameter. Such indications, presently dominated by SK, could be strengthened by further K2K data, provided that the current spectral features are confirmed with higher statistics. A detailed description of the statistical analysis of SK and K2K data is also given, using the so-called ``pull'' approach to systematic uncertainties.Comment: 18 pages (RevTeX) + 12 figures (PostScript

    Probing the LSND scale and four neutrino scenarios with a neutrino telescope

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    We show in this paper that the observation of the angular distribution of upward-going muons and cascade events induced by atmospheric neutrinos at the TeV energy scale, which can be performed by a kilometer-scale neutrino telescope, such as the IceCube detector, can be used to probe a large neutrino mass splitting, Δm2(0.52.0)| \Delta m^2 | \sim (0.5-2.0) eV2^2, implied by the LSND experiment and discriminate among four neutrino mass schemes. This is due to the fact that such a large mass scale can promote non negligible muon neutrino to electron/tau neutrino (and/or anti-muon neutrino to anti-electron/anti-tau neutrino) conversions at these energies by the MSW effect as well as vacuum oscillation, unlike what is expected if all the neutrino mass splittings are small.Comment: LATEX file, with 9 pages, and 4 figures. Update version with one new figur

    Rephasing Invariants of CP and T Violation in the Four-Neutrino Mixing Models

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    We calculate the rephasing invariants of CP and T violation in a favorable parametrization of the 4x4 lepton flavor mixing matrix. Their relations with the CP- and T-violating asymmetries in neutrino oscillations are derived, and the matter effects are briefly discussed.Comment: RevTex 9 pages. Slight changes. Phys. Rev. D (in press

    Neutrino Mass Spectrum and Future Beta Decay Experiments

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    We study the discovery potential of future beta decay experiments on searches for the neutrino mass in the sub-eV range, and, in particular, KATRIN experiment with sensitivity m>0.3m > 0.3 eV. Effects of neutrino mass and mixing on the beta decay spectrum in the neutrino schemes which explain the solar and atmospheric neutrino data are discussed. The schemes which lead to observable effects contain one or two sets of quasi-degenerate states. Future beta decay measurements will allow to check the three neutrino scheme with mass degeneracy, moreover, the possibility appears to measure the CP-violating Majorana phase. Effects in the four neutrino schemes which can also explain the LSND data are strongly restricted by the results of Bugey and CHOOZ oscillation experiments: Apart from bending of the spectrum and the shift of the end point one expects appearance of small kink of (<2 < 2% ) size or suppressed tail after bending of the spectrum with rate below 2 % of the expected rate for zero neutrino mass. We consider possible implications of future beta decay experiments for the neutrino mass spectrum, the determination of the absolute scale of neutrino mass and for establishing the nature of neutrinos. We show that beta decay measurements in combination with data from the oscillation and double beta decay experiments will allow to establish the structure of the scheme (hierarchical or non-hierarchical), the type of the hierarchy or ordering of states (normal or inverted) and to measure the relative CP-violating phase in the solar pair of states.Comment: 48 pages, LaTeX, 8 figures, typos removed, references and discussion of the supernova neutrino bounds adde
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