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The determination of the neutrino mass ordering is currently pursued by several experiments and proposals. A very challenging one is its evaluation from reactor experiments based on the tiny interference effect between the $\Delta m^2_{31}$…

High Energy Physics - Phenomenology · Physics 2017-12-20 Luca Stanco , Giuseppe Salamanna , Alexey Lokhov , Fatma Sawy , Chiara Sirignano

Two-loop radiative mechanism, when combined with an U(1)_{L'} symmetry generated by L_e-L_\mu-L_\tau (=L'), is shown to provide an estimate of \Delta m^2_{\odot}/\Delta m^2_{atm} $\sim$ \epsilon m_e/m_\tau, where \epsilon measures the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Teruyuki Kitabayashi , Masaki Yasue

In recent Letter by An et al. [arXiv:1203.1669] Daya Bay measurements of non-zero value for the neutrino mixing angle {\theta}_{13} with a significance of 5.2 standard deviations were reported. The value of sin^2 {\theta}_{13} was…

High Energy Physics - Phenomenology · Physics 2012-05-01 V. D. Rusov , V. A. Tarasov , S. A. Chernegenko , V. P. Smolyar

The strange quark contribution to proton's spin ($\Delta s$) is a fundamental quantity that is poorly determined from current experiments. Neutrino-proton elastic scattering (pES) is a promising channel to measure this quantity, and…

High Energy Physics - Phenomenology · Physics 2022-11-17 Bhavesh Chauhan

Searches for a light sterile neutrino have been performed independently by the MINOS and the Daya Bay experiments using the muon (anti)neutrino and electron antineutrino disappearance channels, respectively. In this Letter, results from…

High Energy Physics - Experiment · Physics 2016-10-18 Daya Bay , MINOS Collaborations , : , P. Adamson , F. P. An , I. Anghel , A. Aurisano , A. B. Balantekin , H. R. Band , G. Barr , M. Bishai , A. Blake , S. Blyth G. J. Bock , D. Bogert , D. Cao , G. F. Cao , J. Cao , S. V. Cao , T. J. Carroll , C. M. Castromonte , W. R. Cen , Y. L. Chan , J. F. Chang , L. C. Chang , Y. Chang , H. S. Chen , Q. Y. Chen , R. Chen , S. M. Chen , Y. Chen , Y. X. Chen , J. Cheng , J. -H. Cheng , Y. P. Chen , Z. K. Cheng , J. J. Cherwinka , S. Childress , M. C. Chu , A. Chukanov , J. A. B. Coelho , L. Corwin , D. Cronin-Hennessy , J. P. Cummings , J. de Arcos , S. De Rijck , Z. Y. Deng , A. V. Devan , N. E. Devenish , X. F. Ding , Y. Y. Ding , M. V. Diwan , M. Dolgareva , J. Dove , D. A. Dwyer , W. R. Edwards , C. O. Escobar , J. J. Evans , E. Falk , G. J. Feldman , W. Flanagan , M. V. Frohne , M. Gabrielyan , H. R. Gallagher , S. Germani , R. Gill , R. A. Gomes , M. Gonchar , G. H. Gong , H. Gong , M. C. Goodman , P. Gouffon , N. Graf , R. Gran , M. Grassi , K. Grzelak , W. Q. Gu , M. Y. Guan , L. Guo , R. P. Guo , X. H. Guo , Z. Guo , A. Habig , R. W. Hackenburg , S. R. Hahn , R. Han , S. Hans , J. Hartnell , R. Hatcher , M. He , K. M. Heeger , Y. K. Heng , A. Higuera , A. Holin , Y. K. Hor , Y. B. Hsiung , B. Z. Hu , T. Hu , W. Hu , E. C. Huang , H. X. Huang , J. Huang , X. T. Huang , P. Huber , W. Huo , G. Hussain , J. Hylen , G. M. Irwin , Z. Isvan , D. E. Jaffe , P. Jaffke , C. James , K. L. Jen , D. Jensen , S. Jetter , X. L. Ji , X. P. Ji , J. B. Jiao , R. A. Johnson , J. K. de Jong , J. Joshi , T. Kafka , L. Kang , S. M. S. Kasahara , S. H. Kettell , S. Kohn , G. Koizumi , M. Kordosky , M. Kramer , A. Kreymer , 1 K. K. Kwan , M. W. Kwok , T. Kwok , K. Lang , T. J. Langford , K. Lau , L. Lebanowski , J. Lee , J. H. C. Lee , R. T. Lei , R. Leitner , J. K. C. Leung , C. Li , D. J. Li , F. Li , G. S. Li , Q. J. Li , S. Li , S. C. Li , W. D. Li , X. N. Li , Y. F. Li , Z. B. Li , H. Liang , C. J. Lin , G. L. Lin , S. Lin , S. K. Lin , Y. -C. Lin , J. J. Ling J. M. Link , P. J. Litchfield , L. Littenberg , B. R. Littlejohn , D. W. Liu , J. C. Liu , J. L. Liu , C. W. Loh , C. Lu , H. Q. Lu , J. S. Lu , P. Lucas , K. B. Luk , Z. Lv , Q. M. Ma , X. B. Ma , X. Y. Ma , Y. Q. Ma , Y. Malyshkin , W. A. Mann , M. L. Marshak , D. A. Martinez Caicedo , N. Mayer , K. T. McDonald , C. McGivern , R. D. McKeown , M. M. Medeiros , R. Mehdiyev , J. R. Meier , M. D. Messier , W. H. Miller , S. R. Mishra , I. Mitchell , M. Mooney , C. D. Moore , L. Mualem , J. Musser , Y. Nakajima , D. Naples , J. Napolitano , D. Naumov , E. Naumova , J. K. Nelson , H. B. Newman , H. Y. Ngai , R. J. Nichol , Z. Ning , A. Nowak , J. O'Connor , J. P. Ochoa-Ricoux , A. Olshevskiy , M. Orchanian , R. , R. B. Pahlka , J. Paley , H. -R. Pan , J. Park , R. B. Patterson , S. Patton , G. Pawloski , V. Pec , J. C. Peng , A. Perch , M. M. Pfutzner , D. D. Phan , S. Phan-Budd , L. Pinsky , R. K. Plunkett , N. Poonthottathil , C. S. J. Pun , F. Z. Qi , M. Qi , X. Qian , X. Qiu , A. Radovic , N. Raper , B. Rebel , J. Ren , C. Rosenfeld , R. Rosero , B. Roskovec , X. C. Ruan , H. A. Rubin , P. Sail , M. C. Sanchez , J. Schneps , A. Schreckenberger , P. Schreiner , R. Sharma , S. Moed Sher , A. Sousa , H. Steiner , G. X. Sun , J. L. Sun , N. Tagg , R. L. Talaga , W. Tang , D. Taychenachev , J. Thomas , M. A. Thomson , X. Tian A. Timmons , J. Todd , S. C. Tognini , R. Toner , D. Torretta , K. Treskov , K. V. Tsang , C. E. Tull , G. Tzanakos , J. Urheim , P. Vahle , N. Viaux , B. Viren , V. Vorobel , C. H. Wang , M. Wang , N. Y. Wang , R. G. Wang , W. Wang , X. Wang , Y. F. Wang , Z. Wang , Z. M. Wang , R. C. Webb , A. Weber , H. Y. Wei , L. J. Wen , K. Whisnant , C. White , L. Whitehead L. H. Whitehead , T. Wise , S. G. Wojcicki , H. L. H. Wong , S. C. F. Wong , E. Worcester , C. -H. Wu , Q. Wu , W. J. Wu , D. M. Xia , J. K. Xia , Z. Z. Xing , J. L. Xu , J. Y. Xu , Y. Xu , T. Xue , C. G. Yang , H. Yang , L. Yang , M. S. Yang , M. T. Yang , M. Ye. , Z. Ye , M. Yeh , B. L. Young , Z. Y. Yu , S. Zeng , L. ZhanC. Zhang , H. H. Zhang , J. W. Zhang , Q. M. Zhang , X. T. Zhang , Y. M. Zhang , Y. X. Zhang , Z. J. Zhang , Z. P. Zhang , Z. Y. Zhang , J. Zhao , Q. W. Zhao , Y. B. Zhao , W. L. Zhong , L. Zhou , N. Zhou , H. L. Zhuang , J. H. Zou

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

In the past decades, short baseline neutrino oscillation studies around experimental or commercial reactor cores have revealed two anomalies. The first one is linked to the absolute flux and the second one to the spectral shape. The first…

High Energy Physics - Experiment · Physics 2019-05-29 Laura Bernard

The Reactor Experiment for Neutrino Oscillation (RENO) has been taking electron antineutrino ($\overline{\nu}_{e}$) data from the reactors in Yonggwang, Korea, using two identical detectors since August 2011. Using roughly 500 live days of…

The search for neutrinoless double beta decay ($0\nu\beta\beta$) is currently one of the key objectives in neutrino physics research. The decay rate of $0\nu\beta\beta$ decay depends on the effective Majorana neutrino mass $|\langle m…

High Energy Physics - Phenomenology · Physics 2026-01-28 Prokash Pegu , Chandan Duarah

The far site detector complex of the Daya Bay reactor experiment is proposed as a location to search for sterile neutrinos with > eV mass. Antineutrinos from a 500 kCi 144Ce-144Pr beta-decay source (DeltaQ=2.996 MeV) would be detected by…

High Energy Physics - Experiment · Physics 2013-05-08 D. A. Dwyer , K. M. Heeger , B. R. Littlejohn , P. Vogel

The sensitivity to the sterile neutrino mixing at very short baseline reactor neutrino experiments is investigated. In the case of conventional (thermal neutron) reactors it is found that the sensitivity is lost for $\Delta m^2 \gtrsim$ 1…

High Energy Physics - Phenomenology · Physics 2011-09-13 Osamu Yasuda

We discuss short-baseline electron and muon neutrino disappearance searches into sterile neutrinos at a Very Low Energy Neutrino Factory (VLENF) with a muon energy between about two and four GeV. A lesson learned from reactor experiments,…

High Energy Physics - Phenomenology · Physics 2013-05-30 Walter Winter

Recent studies of atmospheric neutrinos and the results from CHOOZ and Palo-Verde experiment call for new and more sensitive searches for neutrino oscillations at reactors. The main goal of the project considered here is to look for very…

High Energy Physics - Experiment · Physics 2009-10-31 L. Mikaelyan

The pattern of oscillation parameters emerging from current experimental data can be further elucidated by the observation of matter effects. In contrast to planned experiments with conventional neutrino beams, atmospheric neutrinos offer…

High Energy Physics - Phenomenology · Physics 2011-09-13 T. Tabarelli de Fatis

We propose an experiment to test the hypothesis that the reported anomaly on atmospheric neutrino fluxes is due to nu_mu <-> nu_x oscillations. It will rely both on a disappearance technique, exploiting the method of the dependence of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Curioni , G. Mannocchi , L. Periale , P. Picchi , F. Pietropaolo , S. Ragazzi

We report first results of a search for the non-zero neutrino mixing angle \theta_{13} from the Double Chooz experiment. Double Chooz aims to measure the mixing angle based on anti-electron-neutrino disappearance as a consequence of…

High Energy Physics - Experiment · Physics 2019-08-13 Tsunayuki Matsubara

There is accumulating evidence for a difference between neutrino and antineutrino oscillations at the $\sim 1$ eV$^2$ scale. The MiniBooNE experiment observes an unexplained excess of electron-like events at low energies in neutrino mode,…

The Daya Bay Reactor Neutrino Experiment has measured a non-zero value of the neutrino mixing angle $\theta_{13}$ with a significance of 7.7 standard deviations by a rate-only a nalysis. The distortion of neutrino energy spectrum carries…

Instrumentation and Detectors · Physics 2015-06-19 Masheng Yang , Yaping Cheng

Neutrino oscillation models involving extra mass eigenstates beyond the standard three (3+N) are fit to global short baseline experimental data. We find that 3+1 has a best fit of Delta m^2_41 = 1.75 eV^2 with a Delta chi^2 [null-min] (dof)…

High Energy Physics - Phenomenology · Physics 2016-06-22 G. H. Collin , C. A. Argüelles , J. M. Conrad , M. H. Shaevitz

There is an observed deficit of about 6\% in the expected rate of anti-neutrino interactions when averaging over many different reactor experiments. While the significance of the deficit is low (98.6 \% CL), there is speculation that a…

High Energy Physics - Experiment · Physics 2015-01-06 M. Bergevin , C. Grant , R. Svoboda