English
Related papers

Related papers: Reactor antineutrino experiments

200 papers

This paper discusses recent results and near-term prospects of the long-baseline neutrino experiments MINOS, MINOS+, T2K and NOvA. The non-zero value of the third neutrino mixing angle {\theta}13 allows experimental analysis in a manner…

High Energy Physics - Experiment · Physics 2016-02-17 Tsuyoshi Nakaya , Robert K. Plunkett

The Daya Bay Reactor Neutrino Experiment has measured a non-zero value for the neutrino mixing angle $\theta_{13}$ with a significance of 5.2 standard deviations. Antineutrinos from six 2.9 GW$_{\rm th}$ reactors were detected in six…

High Energy Physics - Experiment · Physics 2012-10-29 F. P. An , J. Z. Bai , A. B. Balantekin , H. R. Band , D. Beavis , W. Beriguete , M. Bishai , S. Blyth , K. Boddy , R. L. Brown , B. Cai , G. F. Cao , J. Cao , R. Carr , W. T. Chan , J. F. Chang , Y. Chang , C. Chasman , H. S. Chen , H. Y. Chen , S. J. Chen , S. M. Chen , X. C. Chen , X. H. Chen , X. S. Chen , Y. Chen , Y. X. Chen , J. J. Cherwinka , M. C. Chu , J. P. Cummings , Z. Y. Deng , Y. Y. Ding , M. V. Diwan , L. Dong , E. Draeger , X. F. Du , D. A. Dwyer , W. R. Edwards , S. R. Ely , S. D. Fang , J. Y. Fu , Z. W. Fu , L. Q. Ge , V. Ghazikhanian , R. L. Gill , J. Goett , 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 , 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 , Z. Isvan , 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 , J. Lee , M. K. P. Lee , R. Leitner , J. K. C. Leung , K. Y. Leung , C. A. Lewis , B. Li , 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 , J. 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 , C. Liu , D. W. Liu , H. Liu , J. C. Liu , J. L. Liu , S. Liu , X. Liu , Y. B. Liu , C. Lu , H. Q. Lu , A. Luk , K. B. Luk , T. Luo , X. L. Luo , L. H. Ma , Q. M. Ma , X. B. Ma , X. Y. Ma , Y. Q. Ma , B. Mayes , K. T. McDonald , M. C. McFarlane , R. D. McKeown , Y. Meng , D. Mohapatra , J. E. Morgan , 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 , D. Oh , A. Olshevski , A. Pagac , S. Patton , C. Pearson , V. Pec , J. C. Peng , L. E. Piilonen , L. Pinsky , C. S. J. Pun , F. Z. Qi , M. Qi , X. Qian , N. Raper , 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 , H. Themann , Y. Torun , S. Trentalange , O. Tsai , K. V. Tsang , R. H. M. Tsang , C. Tull , B. Viren , S. Virostek , V. Vorobel , C. H. Wang , L. S. Wang , L. Y. Wang , L. Z. Wang , M. Wang , N. Y. Wang , R. G. Wang , T. Wang , W. Wang , X. 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 , C. A. Whitten , J. Wilhelmi , T. Wise , H. C. Wong , H. L. H. Wong , J. Wong , E. T. Worcester , F. F. Wu , Q. Wu , D. M. Xia , S. T. Xiang , Q. Xiao , Z. Z. Xing , G. Xu , J. Xu , J. Xu , J. L. Xu , W. Xu , Y. Xu , T. Xue , C. G. Yang , L. Yang , M. Ye , M. Yeh , Y. S. Yeh , K. Yip , B. L. Young , Z. Y. Yu , L. Zhan , C. Zhang , F. H. Zhang , J. W. Zhang , Q. M. Zhang , K. Zhang , Q. X. Zhang , S. H. Zhang , Y. C. Zhang , Y. H. Zhang , Y. X. Zhang , Z. J. Zhang , Z. P. Zhang , Z. Y. Zhang , J. Zhao , Q. W. Zhao , Y. B. Zhao , L. Zheng , W. L. Zhong , L. Zhou , Z. Y. Zhou , H. L. Zhuang , J. H. Zou

Most of the neutrino oscillation results can be explained by the three-neutrino paradigm. However several anomalies in short baseline oscillation data could be interpreted by invoking a hypothetical fourth neutrino, separated from the three…

High Energy Physics - Experiment · Physics 2014-10-09 Thierry Lasserre

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 SNO+ collaboration reports its second spectral analysis of reactor antineutrino oscillation using 286 tonne-years of new data. The measured energies of reactor antineutrino candidates were fitted to obtain the second-most precise…

High Energy Physics - Experiment · Physics 2025-09-18 SNO+ Collaboration , : , M. Abreu , V. Albanese , A. Allega , R. Alves , M. R. Anderson , S. Andringa , L. Anselmo , J. Antunes , E. Arushanova , S. Asahi , M. Askins , D. M. Asner , D. J. Auty , A. R. Back , S. Back , A. Bacon , T. Baltazar , F. Barão , Z. Barnard , A. Barr , N. Barros , D. Bartlett , R. Bayes , C. Beaudoin , E. W. Beier , G. Berardi , T. S. Bezerra , A. Bialek , S. D. Biller , E. Blucher , A. Boeltzig , R. Bonventre , M. Boulay , D. Braid , E. Caden , E. J. Callaghan , J. Caravaca , J. Carvalho , L. Cavalli , D. Chauhan , M. Chen , S. Cheng , O. Chkvorets , K. J. Clark , B. Cleveland , C. Connors , D. Cookman , J. Corning , I. T. Coulter , M. A. Cox , D. Cressy , X. Dai , C. Darrach , S. DeGraw , R. Dehghani , J. Deloye , M. M. Depatie , F. Descamps , C. Dima , J. Dittmer , K. H. Dixon , F. Di Lodovico , A. Doxtator , N. Duhaime , F. Duncan , J. Dunger , A. D. Earle , M. S. Esmaeilian , D. Fabris , E. Falk , A. Farrugia , N. Fatemighomi , C. Felber , V. Fischer , E. Fletcher , R. Ford , K. Frankiewicz , N. Gagnon , A. Gaur , J. Gauthier , A. Gibson-Foster , K. Gilje , O. I. González-Reina , D. Gooding , P. Gorel , K. Graham , C. Grant , J. Grove , S. Grullon , E. Guillian , R. L. Hahn , S. Hall , A. L. Hallin , D. Hallman , S. Hans , J. Hartnell , P. Harvey , C. Hearns , M. R. Hebert , M. Hedayatipour , W. J. Heintzelman , J. Heise , R. L. Helmer , C. Hewitt , B. Hodak , M. Hodak , M. Hood , D. Horne , M. Howe , B. Hreljac , J. Hu , P. Huang , R. Hunt-Stokes , T. Iida , A. S. Inácio , C. M. Jackson , N. A. Jelley , C. J. Jillings , C. Jones , P. G. Jones , S. Kaluzienski , K. Kamdin , T. Kaptanoglu , J. Kaspar , K. Keeter , C. Kefelian , P. Khaghani , L. Kippenbrock , J. Kladnik , J. R. Klein , R. Knapik , J. Kofron , L. L. Kormos , S. Korte , B. Krar , C. Kraus , C. B. Krauss , T. Kroupová , K. Labe , F. Lafleur , C. Lake , I. Lam , C. Lan , B. J. Land , R. Lane , S. Langrock , P. Larochelle , S. Larose , A. LaTorre , I. Lawson , L. Lebanowski , J. Lee , C. Lefebvre , G. M. Lefeuvre , E. J. Leming , A. Li , O. Li , J. Lidgard , B. Liggins , P. Liimatainen , Y. H. Lin , X. Liu , Y. Liu , V. Lozza , M. Luo , S. Maguire , A. Maio , K. Majumdar , S. Manecki , J. Maneira , R. D. Martin , E. Marzec , A. Mastbaum , A. Mathewson , N. McCauley , A. B. McDonald , K. McFarlane , P. Mekarski , M. Meyer , C. Miller , C. Mills , G. Milton , M. Mlejnek , E. Mony , B. Morissette , D. Morris , I. Morton-Blake , M. J. Mottram , M. Mubasher , S. Nae , S. Naugle , M. Newcomer , M. Nirkko , L. J. Nolan , V. M. Novikov , H. M. O'Keeffe , E. O'Sullivan , G. D. Orebi Gann , S. Ouyang , J. Page , S. Pal , K. Paleshi , W. Parker , M. J. Parnell , J. Paton , S. J. M. Peeters , T. Pershing , Z. Petriw , J. Petzoldt , L. J. Pickard , D. Pracsovics , G. Prior , J. C. Prouty , B. Quenallata , S. Quirk , P. Ravi , S. Read , A. Reichold , M. Reinhard , S. Riccetto , M. Rigan , I. Ritchie , A. Robertson , B. C. Robertson , J. Rose , R. Rosero , P. M. Rost , J. Rumleskie , A. Sörensen , P. Schrock , M. A. Schumaker , M. H. Schwendener , D. Scislowski , J. Secrest , M. Seddighin , L. Segui , S. Seibert , I. Semenec , F. Shaker , T. Shantz , M. K. Sharma , J. Shen , T. M. Shokair , L. Sibley , J. Simms , J. R. Sinclair , K. Singh , P. Skensved , M. Smiley , T. Sonley , M. St-Amant , R. Stainforth , S. Stankiewicz , M. Strait , M. I. Stringer , A. Stripay , R. Svoboda , S. Tacchino , R. Tafirout , B. Tam , C. Tanguay , J. Tatar , L. Tian , N. Tolich , J. Tseng , H. W. C. Tseung , E. Turner , E. Vázquez-Jáuregui , S. Valder , R. Van Berg , J. G. C. Veinot , C. J. Virtue , B. von Krosigk , J. M. G. Walker , M. Walker , J. Wallig , S. C. Walton , F. Wang , J. Wang , M. Ward , J. Waterfield , J. J. Weigand , R. F. White , J. F. Wilkerson , J. R. Wilson , J. D. Wilson , T. J. Winchester , P. Woosaree , A. Wright , S. Yang , K. Yazigi , Z. Ye , M. Yeh , S. Yu , T. Zhang , Y. Zhang , T. Zhao , K. Zuber , A. Zummo

I shall sketch the history of reactor neutrino physics over five decades since the Reines-Cowan proof of neutrino existence in the late 50s, till the advent of the present era of precision reactor neutrino oscillation experiments. There are…

High Energy Physics - Phenomenology · Physics 2019-02-13 Petr Vogel

Since the discovery of nuclear beta decay, nuclear physicists have studied the weak interaction and the nature of neutrinos. Many recent and current experiments have been focused on the elucidation of neutrino oscillations and neutrino…

Instrumentation and Detectors · Physics 2014-12-04 R. D. McKeown

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

This article reports the optimized experimental requirements to determine neutrino mass hierarchy using electron antineutrinos ($\bar{\nu}_e$) generated in a nuclear reactor. The features of the neutrino mass hierarchy can be extracted from…

High Energy Physics - Experiment · Physics 2016-01-20 M. Y. Pac

Recently new reactor antineutrino spectra have been provided for 235U, 239Pu, 241Pu and 238U, increasing the mean flux by about 3 percent. To good approximation, this reevaluation applies to all reactor neutrino experiments. The synthesis…

High Energy Physics - Experiment · Physics 2011-05-12 G. Mention , M. Fechner , Th. Lasserre , Th. A. Mueller , D. Lhuillier , M. Cribier , A. Letourneau

The three-flavor neutrino oscillation model describes the well-studied phenomenon of neutrinos produced in association with one charged lepton: electron, muon, or tau, and then later detected in association with a possibly different charged…

High Energy Physics - Phenomenology · Physics 2026-03-25 Peter B. Denton

The Daya Bay and RENO reactor neutrino experiments have revealed that the smallest neutrino mixing angle is in fact relatively large, i.e., theta_13 ~ 9 degrees. Motivated by this exciting progress, we perform a systematic study of the…

High Energy Physics - Phenomenology · Physics 2013-03-29 Xue-wen Liu , Shun Zhou

Neutrino oscillations are clear evidence for physics beyond the standard model. The goal of next-generation neutrino oscillation experiments is to find a non-zero $\theta_{13}$, the last mixing matrix element for which we only know an upper…

High Energy Physics - Experiment · Physics 2008-05-19 Teppei Katori

Despite the dramatic progress made in neutrino oscillation studies recently, several fundamental neutrino parameters remain either unknown or poorly measured. We discuss in detail a method for their measurement by precision studies of…

High Energy Physics - Phenomenology · Physics 2008-11-08 Mikhail Batygov , Stephen Dye , John Learned , Shigenobu Matsuno , Sandip Pakvasa , Gary Varner

The RENO experiment reports more precisely measured values of $\theta_{13}$ and $|\Delta m_{ee}^2|$ using $\sim$2\,200 live days of data. The amplitude and frequency of reactor electron antineutrino ($\overline{\nu}_e$) oscillation are…

We discuss the neutrino oscillations, using texture zero mass matrices for the leptons. The reactor mixing angle $\theta^{}_{l}$ is calculated. The ratio of the masses of two neutrinos is determined by the solar mixing angle. We can…

High Energy Physics - Phenomenology · Physics 2015-06-11 Harald Fritzsch

The Daya Bay Reactor Neutrino Experiment has measured the neutrino mixing angle \theta_{13} to world-leading precision. The experiment uses eight antineutrino detectors filled with 20-tons of gadolinium-doped liquid scintillator to detect…

With the educated, interested non-specialist as the target audience, we overview what is known and not known about contemporary neutrino physics. Theory tells us that neutrinos are the second-most common particle in the Universe, behind…

High Energy Physics - Phenomenology · Physics 2013-08-09 Thomas J Weiler

We analyze neutrino oscillations in a thought experiment in which neutrinos are produced by electrons on target nuclei. The neutrinos are detected through charged lepton production in their collision with nuclei in detector. Both the target…

High Energy Physics - Phenomenology · Physics 2010-04-05 A. D. Dolgov , O. V. Lychkovskiy , A. A. Mamonov , L. B. Okun , M. V. Rotaev , M. G. Schepkin

In this paper, we first discuss the detection of supernova neutrino on Earth. Then we propose a possible method to acquire information about $\theta_{13}$ smaller than $1.5^\circ$ by detecting the ratio of the event numbers of different…

High Energy Physics - Phenomenology · Physics 2010-01-22 Xin-Heng Guo , Ming-Yang Huang , Bing-Lin Young
‹ Prev 1 4 5 6 7 8 10 Next ›