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200 papers

The SNO+ experiment is the follow-up to the Sudbury Neutrino Observatory (SNO). The heavy water that was in SNO will be replaced with a liquid scintillator of linear alkylbenzene (plus fluor). SNO+ has many physics goals including detecting…

High Energy Physics - Experiment · Physics 2019-08-14 Mark C. Chen

Many experiments whose goal is the search for neutrino-less double beta decay are taking data or in a final construction stage. The need for a tool that allows for an objective comparison between the sensitivity of different experiments is…

Instrumentation and Detectors · Physics 2014-02-21 M. Biassoni , O. Cremonesi , P. Gorla

This letter reports results from a search for muon-neutrino to electron-neutrino transitions by the MINOS experiment based on a 7x10^20 protons-on-target exposure. Our observation of 54 candidate electron-neutrino events in the Far Detector…

High Energy Physics - Experiment · Physics 2012-08-27 The MINOS Collaboration

The low energy part of the reactor neutrino spectra has not been experimentally measured. Its uncertainties limit the sensitivities in certain reactor neutrino experiments. The origin of these uncertainties are discussed, and the effects on…

High Energy Physics - Experiment · Physics 2009-09-25 Hau-Bin Li , Henry T. Wong

Conventional reactor neutrino experiments are dissapearance experiments, and thus have less sensitivity to small mixing angles than appearance experiments do. It has been recently shown that future reactor neutrino experiments consisiting…

High Energy Physics - Phenomenology · Physics 2009-11-10 Jose Bernabeu , Sergio Palomares-Ruiz

This presentation describes a precision result of the neutrino mixing parameter, $\sin^2 2\theta_{13}$, and the first direct measurement of the antineutrino mass-squared difference $\sin^2(\Delta_{ee}) \equiv \cos^2 \theta_{12} \sin^2…

High Energy Physics - Experiment · Physics 2019-08-13 Bei-Zhen Hu

This paper presents a strategy for measuring sin^2 theta_W to ~1% at a reactor-based experiment, using antineutrinos electron elastic scattering. This error is comparable to the NuTeV, SLAC E158, and APV results on sin^2 theta_W, but with…

High Energy Physics - Experiment · Physics 2009-11-10 J. M. Conrad , J. M. Link , M. H. Shaevitz

Angle \theta_13 is one of the two unknown neutrino mixing parameters to be determined. Its value may determine the future trend of the neutrino physics. We propose to measure sin^22\theta_13 with a sensitivity better than 0.01 (90% C.L) at…

High Energy Physics - Experiment · Physics 2017-08-23 Yifang Wang

The RENO experiment is a short baseline neutrino experiment in Korea aiming to measure the neutrino mixing angle theta_13 or set limit to sin^2(2 theta_13) less than 0.02. This document describes physics goals, experimental site, detector…

High Energy Physics - Experiment · Physics 2010-03-09 RENO Collaboration , J. K. Ahn

I describe how reactor measurements of $\sin^22\theta_{13}$ can be improved by a near-far detector complex. I show that in the Kashiwazaki plan it is potentially possible to measure $\sin^2{2\theta_{13}}$ down to 0.02.

High Energy Physics - Phenomenology · Physics 2009-11-10 Osamu Yasuda

The RENO experiment recently reported the disappearance of reactor electron antineutrinos consistent with neutrino oscillations, with a significance of 4.9 standard deviations. The published ratio of observed to expected number of…

We investigate the impact of a fourth sterile neutrino at reactor and Spallation Neutron Source neutrino detectors. Specifically, we explore the discovery potential of the TEXONO and COHERENT experiments to subleading sterile neutrino…

High Energy Physics - Phenomenology · Physics 2017-09-26 T. S. Kosmas , D. K. Papoulias , M. Tortola , J. W. F. Valle

Three dedicated reactor experiments, Double Chooz, RENO and Daya Bay, have recently performed a precision measurement of the third standard mixing angle $\theta_{13}$ exploiting a multiple baseline comparison of $\nu_e \to \nu_e$…

High Energy Physics - Phenomenology · Physics 2015-06-17 Antonio Palazzo

Taking into account recent theoretical and experimental inputs on reactor fluxes we reconsider the determination of the weak mixing angle from low energy experiments. We perform a global analysis to all available neutrino-electron…

High Energy Physics - Phenomenology · Physics 2016-09-07 B. C. Canas , E. A. Garces , O. G. Miranda , M. Tortola , J. W. F. Valle

This letter reports on a search for $\nu_\mu \to \nu_e$ transitions by the MINOS experiment based on a \unit[$3.14\times10^{20}$]{protons-on-target} exposure in the Fermilab NuMI beam. We observe 35 events in the Far Detector with a…

High Energy Physics - Experiment · Physics 2012-08-27 MINOS Collaboration

Coherent scattering is a flavor-blind, high-rate, as yet undetected neutrino interaction predicted by the Standard Model. We propose to use a compact (kg-scale), two-phase (liquid-gas) argon ionization detector to measure coherent neutrino…

Nuclear Experiment · Physics 2009-11-10 Chris Hagmann , Adam Bernstein

Presently, there are several experimental setups dedicated to rare event searches, such as dark matter interactions or double beta decay, in the building or commissioning phases. These experiments often use large mass detectors and have…

High Energy Astrophysical Phenomena · Physics 2012-11-08 Carlos Martinez Amaya , Matteo Biassoni

Elegant experiments are being carried out, or are in preparation, to improve the precision with which the solar and atmospheric neutrino-oscillation parameters are known, and to attempt to make a first measurement of the small mixing angle…

Instrumentation and Detectors · Physics 2010-01-05 K. Long

The Daya Bay Reactor Neutrino Experiment is designed to determine precisely the neutrino mixing angle $\theta_{13}$ with a sensitivity better than 0.01 in the parameter sin$^22\theta_{13}$ at the 90% confidence level. To achieve this goal,…

Instrumentation and Detectors · Physics 2012-10-29 Daya Bay Collaboration , F. P. An , Q. An , J. Z. Bai , A. B. Balantekin , H. R. Band , W. Beriguete , M. Bishai , S. Blyth , R. L. Brown , G. F. Cao , J. Cao , R. Carr , J. F. Chang , Y. Chang , C. Chasman , H. S. Chen , S. J. Chen , S. M. Chen , X. C. Chen , X. H. Chen , X. S. Chen , Y. Chen , J. J. Cherwinka , M. C. Chu , J. P. Cummings , Z. Y. Deng , Y. Y. Ding , M. V. Diwan , E. Draeger , X. F. Du , D. Dwyer , W. R. Edwards , S. R. Ely , S. D. Fang , J. Y. Fu , Z. W. Fu , L. Q. Ge , R. L. Gill , M. Gonchar , G. H. Gong , H. Gong , Y. A. Gornushkin , L. S. Greenler , W. Q. Gu , M. Y. Guan , X. H. Guo , R. W. Hackenburg , R. L. Hahn , S. Hans , H. F. Hao , M. He , Q. He , W. S. He , K. M. Heeger , Y. K. Heng , P. Hinrichs , T. H. Ho , Y. K. Hor , Y. B. Hsiung , B. Z. Hu , T. Hu , T. Hu , H. X. Huang , H. Z. Huang , P. W. Huang , X. Huang , X. T. Huang , P. Huber , D. E. Jaffe , S. Jetter , X. L. Ji , X. P. Ji , H. J. Jiang , W. Q. Jiang , J. B. Jiao , R. A. Johnson , L. Kang , S. H. Kettell , M. Kramer , K. K. Kwan , M. W. Kwok , T. Kwok , C. Y. Lai , W. C. Lai , W. H. Lai , K. Lau , L. Lebanowski , M. K. P. Lee , R. Leitner , J. K. C. Leung , K. Y. Leung , C. A. Lewis , F. Li , G. S. Li , J. Li , Q. J. Li , S. F. Li , W. D. Li , X. B. Li , X. N. Li , X. Q. Li , Y. Li , Z. B. Li , H. Liang , C. J. Lin , G. L. Lin , S. K. Lin , S. X. Lin , Y. C. Lin , J. J. Ling , J. M. Link , L. Littenberg , B. R. Littlejohn , B. J. Liu , D. W. Liu , J. C. Liu , J. L. Liu , S. Liu , X. Liu , Y. B. Liu , C. Lu , H. Q. Lu , A. Luk , K. B. Luk , X. L. Luo , L. H. Ma , Q. M. Ma , X. Y. Ma , Y. Q. Ma , B. Mayes , K. T. McDonald , M. C. McFarlane , R. D. McKeown , Y. Meng , D. Mohapatra , Y. Nakajima , J. Napolitano , D. Naumov , I. Nemchenok , C. Newsom , H. Y. Ngai , W. K. Ngai , Y. B. Nie , Z. Ning , J. P. Ochoa-Ricoux , A. Olshevski , A. Pagac , S. Patton , V. Pec , J. C. Peng , L. E. Piilonen , L. Pinsky , C. S. J. Pun , F. Z. Qi , M. Qi , X. Qian , R. Rosero , B. Roskovec , X. C. Ruan , B. Seilhan , B. B. Shao , K. Shih , H. Steiner , P. Stoler , G. X. Sun , J. L. Sun , Y. H. Tam , H. K. Tanaka , X. Tang , Y. Torun , S. Trentalange , O. Tsai , K. V. Tsang , R. H. M. Tsang , C. Tull , B. Viren , V. Vorobel , C. H. Wang , L. S. Wang , L. Y. Wang , M. Wang , N. Y. Wang , R. G. Wang , W. Wang , X. Wang , Y. F. Wang , Z. Wang , Z. Wang , Z. M. Wang , D. M. Webber , Y. D. Wei , L. J. Wen , D. L. Wenman , K. Whisnant , C. G. White , L. Whitehead , J. Wilhelmi , T. Wise , H. L. H. Wong , J. Wong , F. F. Wu , Q. Wu , J. B. Xi , D. M. Xia , Q. Xiao , Z. Z. Xing , G. Xu , J. Xu , J. Xu , J. L. Xu , Y. Xu , T. Xue , C. G. Yang , L. Yang , M. Ye , M. Yeh , Y. S. Yeh , B. L. Young , Z. Y. Yu , L. Zhan , C. Zhang , F. H. Zhang , J. W. Zhang , Q. M. Zhang , S. H. Zhang , Y. C. Zhang , Y. H. Zhang , Y. X. Zhang , Z. J. Zhang , Z. P. Zhang , Z. Y. Zhang , H. Zhao , J. Zhao , Q. W. Zhao , Y. B. Zhao , L. Zheng , W. L. Zhong , L. Zhou , Y. Z. Zhou , Z. Y. Zhou , H. L. Zhuang , J. H. Zou

The lepton mixing angle theta_13, the only unknown angle in the standard three-flavor neutrino mixing scheme, is finally measured by the recent reactor and accelerator neutrino experiments. We perform a combined analysis of the data coming…

High Energy Physics - Phenomenology · Physics 2015-06-03 P. A. N. Machado , H. Minakata , H. Nunokawa , R. Zukanovich Funchal