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Related papers: Double-Chooz: a search for Theta13

200 papers

Until recently, measurements of theta_13, which describes the nu_e component in the nu_3 mass eigenstate, gave only upper limits, leaving open the possibility that it is zero and eliminating a source of CP violation in the neutrino sector.…

High Energy Physics - Experiment · Physics 2011-11-11 D. Karlen

Reactor neutrinos play an important role in determining parameter theta_{13} in the lepton mixing (PMNS) matrix. A next important step on measuring PMNS matrix could be to build another reactor neutrino experiment, for example, DaYa bay in…

High Energy Physics - Phenomenology · Physics 2009-01-16 Q. Y. Liu , J. Deng , B. L. Chen , P. Yang

The possibility to improve the CERN to Gran Sasso neutrino beam performances for theta_{13} searches is investigated. We show that by an appropriate optimization of the target and focusing optics of the present CNGS design, we can increase…

High Energy Physics - Phenomenology · Physics 2009-11-07 A. Rubbia , P. Sala

The technical breakthroughs of multiple detectors developed by Daya Bay and RENO collaborations have gotten great attention. Yet the optimal determination of neutrino mixing parameters from reactor data depends on the statistical method and…

High Energy Physics - Phenomenology · Physics 2014-09-23 Amir N. Khan , Douglas W. McKay , John P. Ralston

The NOMAD experiment has been designed to search for neutrino-tau appearance in the CERN wide-band neutrino beam . The detector is now completed and has been further improved. All subdetectors are working well. The experiment, where the…

High Energy Physics - Phenomenology · Physics 2010-12-23 Marco Laveder

The next-generation Enriched Xenon Observatory (nEXO) is a proposed experiment to search for neutrinoless double beta ($0\nu\beta\beta$) decay in $^{136}$Xe with a target half-life sensitivity of approximately $10^{28}$ years using…

Nuclear Experiment · Physics 2018-10-23 nEXO Collaboration , J. B. Albert , G. Anton , I. J. Arnquist , I. Badhrees , P. S. Barbeau , D. Beck , V. Belov , F. Bourque , J. P. Brodsky , E. Brown , T. Brunner , A. Burenkov , G. F. Cao , L. Cao , W. R. Cen , C. Chambers , S. A. Charlebois , M. Chiu , B. Cleveland , M. Coon , M. Côté , A. Craycraft , W. Cree , J. Dalmasson , T. Daniels , S. J. Daugherty , J. Daughhetee , R. DeVoe , S. Delaquis , A. Der Mesrobian-Kabakian , T. Didberidze , J. Dilling , Y. Y. Ding , M. J. Dolinski , A. Dragone , L. Fabris , W. Fairbank , J. Farine , S. Feyzbakhsh , R. Fontaine , D. Fudenberg , G. Giacomini , R. Gornea , K. Graham , G. Gratta , E. V. Hansen , D. Harris , M. Hasan , M. Heffner , E. W. Hoppe , J. Hößl , A. House , P. Hufschmidt , M. Hughes , Y. Ito , A. Iverson , A. Jamil , M. J. Jewell , X. S. Jiang , T. N. Johnson , S. Johnston , A. Karelin , L. J. Kaufman , R. Killick , T. Koffas , S. Kravitz , R. Krücken , A. Kuchenkov , K. S. Kumar , Y. Lan , D. S. Leonard , G. Li , S. Li , Z. Li , C. Licciardi , Y. H. Lin , R. MacLellan , T. Michel , B. Mong , D. C. Moore , K. Murray , R. J. Newby , Z. Ning , O. Njoya , F. Nolet , K. Odgers , A. Odian , M. Oriunno , J. L. Orrell , G. S. Ortega , I. Ostrovskiy , C. T. Overman , S. Parent , A. Piepke , A. Pocar , J. -F. Pratte , D. Qiu , V. Radeka , E. Raguzin , T. Rao , S. Rescia , F. Retière , A. Robinson , T. Rossignol , P. C. Rowson , N. Roy , R. Saldanha , S. Sangiorgio , S. Schmidt , J. Schneider , A. Schubert , D. Sinclair , K. Skarpaas VIII , A. K. Soma , G. St-Hilaire , V. Stekhanov , T. Stiegler , X. L. Sun , M. Tarka , J. Todd , T. Tolba , R. Tsang , T. Tsang , F. Vachon , V. Veeraraghavan , G. Visser , P. Vogel , J. -L. Vuilleumier , M. Wagenpfeil , Q. Wang , M. Weber , W. Wei , L. J. Wen , U. Wichoski , G. Wrede , S. X. Wu , W. H. Wu , L. Yang , Y. -R. Yen , O. Zeldovich , J. Zettlemoyer , X. Zhang , J. Zhao , Y. Zhou , T. Ziegler

The recent measurement of a non-zero neutrino mixing angle $\theta_{13}$ requires a modification of the tri-bimaximal mixing pattern that predicts a zero value for it. We propose a new neutrino mixing pattern based on a spontaneously-broken…

High Energy Physics - Phenomenology · Physics 2013-05-30 Y. H. Ahn , Seungwon Baek , Paolo Gondolo

A search for pair production of neutral color-octet weak-triplet scalar particles (Theta) is performed in processes where one Theta decays to a pair of b quark jets and the other to a Z boson plus a jet, with the Z boson decaying to a pair…

High Energy Physics - Experiment · Physics 2015-11-02 CMS Collaboration

Till 2010 we had three unknown parameters of neutrino oscillation: the third mixing angle {\theta}_(13), the sign of the larger mass difference {\Delta}m^(2)_(31) and the CP violating phase {\delta}. Thanks to a number of consistent…

High Energy Physics - Phenomenology · Physics 2015-06-16 D. P. Roy

If the lepton mixing angle theta_{23} is not maximal, there arises a problem of ambiguity in determining theta_{23} due to the existence of two degenerate solutions, one in the first and the other in the second octant. We discuss an…

We investigate a relation among neutrino observables, three mixing angles and two mass squared differences, from a cascade texture of neutrino mass matrix. We show an allowed region of the correlation by use of current data of neutrino…

High Energy Physics - Phenomenology · Physics 2011-08-17 Naoyuki Haba , Ryo Takahashi

Neutrino oscillations were discovered by atmospheric and solar neutrino experiments, and have been confirmed by experiments using neutrinos from accelerators and nuclear reactors. It has been found that there are large mixing angles in the…

High Energy Physics - Experiment · Physics 2009-10-23 Trung Le

The recent results from T2K and MINOS experiments point towards a relatively large value of the reactor angle \theta_13 in the lepton sector. In this paper we show how a large \theta_13 can arise from the charged lepton sector alone in the…

High Energy Physics - Phenomenology · Physics 2011-11-22 David Marzocca , Serguey T. Petcov , Andrea Romanino , Martin Spinrath

The disappearance of reactor antineutrinos in the Double Chooz experiment is used to investigate the possibility of neutrino-antineutrino oscillations arising due to the breakdown of Lorentz invariance. We find no evidence for this…

High Energy Physics - Experiment · Physics 2015-06-16 J. S. Diaz , T. Katori , J. Spitz , J. M. Conrad

We introduce a new texture for neutrino mixing named Tri-Permuting (TP) mixing matrix. This pattern is characterized by maximal solar and atmospheric angles and by a large reactor angle satisfying sin(theta_13)=1/3. The correct lepton…

High Energy Physics - Phenomenology · Physics 2015-03-19 F. Bazzocchi

Pioneering atmospheric muon neutrino experiments have demonstrated the near-maximal magnitude of the flavor mixing angle $\theta_{23}$. But the precise value of the deviation $D \equiv 1/2 - \sin^2 \theta_{23}$ from maximality (if nonzero)…

High Energy Physics - Phenomenology · Physics 2009-11-11 Sandhya Choubey , Probir Roy

From the analyses of the recent data of neutrino oscillation experiments (especially the CHOOZ and the Super KAMIOKANDE experiments), we discuss how these data affect the neutrinoless double beta decay ($(\beta \beta)_{0\nu}$) rate and vice…

High Energy Physics - Phenomenology · Physics 2009-10-31 T. Fukuyama , K. Matsuda , H. Nishiura

We study the possibility to measure sin^2 theta_W by neutrino-electron scattering at a value of the momentum transfer Q ~ 30 MeV with a precision of 0.24% which is only a factor three below the one obtained by LEP-I at the Z-pole. The…

High Energy Physics - Phenomenology · Physics 2011-08-29 Sanjib Kumar Agarwalla , Patrick Huber

We discuss the neutrino oscillations, using texture zero mass matrices for the leptons, including radiative correction. The neutrino mixing angle theta_13 is calculated and agrees with the result of the new Daya Bay experiment.

High Energy Physics - Phenomenology · Physics 2015-06-04 Harald Fritzsch

The sensitivity of future neutrino oscillation experiments is determined within a frequentist framework by using a statistical procedure based on Monte Carlo simulations. I consider the search for a non-zero value of the mixing angle…

High Energy Physics - Phenomenology · Physics 2008-11-26 Thomas Schwetz