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We discuss the minimum requirements for a neutrino beta beam if theta_13 is discovered by an upcoming reactor experiment, such as Double Chooz or Daya Bay. We require that both neutrino mass hierarchy and leptonic CP violation can be…

High Energy Physics - Phenomenology · Physics 2009-11-13 Walter Winter

The NEMO experiment is investigating the neutrinoless double beta decay. The NEMO-3 detector is taking data in the Frejus Underground Laboratory. The goal of the SuperNEMO detector is to reach a sensitivity on the order of 10^26 year on the…

High Energy Physics - Experiment · Physics 2008-10-06 Laurent Simard

The Double Chooz reactor-based oscillation experiment searches for an electron antineutrino disappearance signal to investigate the neutrino mass matrix mixing angle theta 13. Double Chooz's reported evidence for this disappearance is…

High Energy Physics - Phenomenology · Physics 2017-08-23 Teppei Katori , Joshua Spitz

The MINOS experiment observes the NuMI beam produced by the Main Injector accelerator at two detector stations, one 1 km and the other 735 km from the neutrino production target. From the disappearance of neutrinos in flight between the two…

High Energy Physics - Experiment · Physics 2019-08-13 Patricia Vahle

It is suggested that a large deep underocean (or ice) neutrino detector, given the presence of significant numbers of neutrinos in the PeV energy range as predicted by various models of Active Galactic Nuclei, can make unique measurements…

High Energy Physics - Phenomenology · Physics 2010-11-01 John G. Learned , Sandip Pakvasa

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

Several efforts are ongoing for the development of spherical gaseous time projection chamber detectors for the observation of rare phenomena such as weakly interacting massive particles or neutrino interactions. The proposed detector,…

We study the optimization of a green-field, two-baseline reactor experiment with respect to the sensitivity for electron antineutrino disappearance in search of a light sterile neutrino. We consider both commercial and research reactors and…

High Energy Physics - Phenomenology · Physics 2022-02-16 Jeffrey M. Berryman , Luis A. Delgadillo , Patrick Huber

Reactor neutrinos play a substantial role in the study of the fundamental properties of neutrinos. With current and upcoming precision experiments, it is essential more than ever to understand the reactor neutrino flux and spectrum.…

Instrumentation and Detectors · Physics 2018-04-03 Bedrich Roskovec

Medium baseline reactor experiments (Double Chooz, Daya Bay and RENO) provide a unique opportunity to test the presence of light sterile neutrinos. We analyze the data of these experiments in the search of sterile neutrinos and also test…

High Energy Physics - Phenomenology · Physics 2013-11-13 Arman Esmaili , Ernesto Kemp , O. L. G. Peres , Zahra Tabrizi

The measurement of the neutrino mixing angle $\theta_{13}$ opens a gateway for the next generation experiments to measure the neutrino mass hierarchy and the leptonic CP-violating phase. Future reactor experiments will focus on mass…

Instrumentation and Detectors · Physics 2013-10-29 Miao He

The purpose of the present paper is to study the neutrino oscillations as they may appear in the low energy neutrinos emitted in triton decay, with maximum neutrino energy of 18.6 KeV. Such low energy neutrino oscillations can only be…

High Energy Physics - Phenomenology · Physics 2007-05-23 Y. Giomataris , J. D. Vergados

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

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

DUNE is an international project, currently in its design phase, for neutrino physics and proton-decay searches. It will consist of two detectors exposed to a megawatt-scale muon neutrino beam that will be produced at Fermilab (Illinois,…

High Energy Physics - Experiment · Physics 2017-10-26 Justo Martín-Albo

A novel low-energy neutrino-oscillation experiment NOSTOS, combining a strong tritium source and a high pressure spherical TPC detector (10 m in radius) has been recently proposed. The goal of the experiment is to measure the mixing angle…

High Energy Physics - Experiment · Physics 2009-11-11 I. Giomataris , S. Aune , P. Colas , I. Irastorza , B. Peyaud , J. Dolbeau , P. Gorodetzky , H. van der Graff , T. Patzak , P. Salin , V. Lepeltier , J. D. Vergados

We revisit correlations of neutrino oscillation parameters in reactor and long-baseline neutrino oscillation experiments. A framework based on an effective value of $\theta_{13}$ is presented, which can easily reproduce experimental…

High Energy Physics - Phenomenology · Physics 2018-04-25 Manfred Lindner , Werner Rodejohann , Xun-Jie Xu

We investigate the determination of neutrino oscillation parameters by experiments within the next ten years. The potential of conventional beam experiments (MINOS, ICARUS, OPERA), superbeam experiments (T2K, NOvA), and reactor experiments…

High Energy Physics - Phenomenology · Physics 2009-11-10 P. Huber , M. Lindner , M. Rolinec , T. Schwetz , W. Winter

It is suggested that a large deep underocean neutrino detector, given the presence of significant numbers of neutrinos in the PeV range as predicted by various models of Active Galactic Nuclei, can make unique measurements of the properties…

High Energy Physics - Phenomenology · Physics 2010-11-01 John G. Learned , Sandip Pakvasa

The last unknown neutrino mixing angle $\theta_{13}$ is one of the fundamental parameters of nature; it is also a crucial parameter for determining the sensitivity of future long-baseline experiments aimed to study CP violation in the…

High Energy Physics - Experiment · Physics 2019-08-13 Cheng-Ju Lin