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One of the main goals of RENO (Reactor Experiment for Neutrino Oscillation) is to measure the smallest neutrino mixing angle {\theta}13 using reactor neutrinos in Korea. RENO is the first reactor experiment taking data with two identical…

High Energy Physics - Experiment · Physics 2019-08-21 Seon-Hee Seo

Muon colliders provide an exciting new direction to expand the energy frontier of particle physics. We point out a new use of these facilities for neutrino and beyond the Standard Model physics using their main detectors. Muon decays along…

High Energy Physics - Phenomenology · Physics 2025-07-31 Luc Bojorquez-Lopez , Matheus Hostert , Carlos A. Argüelles , Zhen Liu

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 OPERA experiment at the CNGS beam has observed muon to tau neutrino oscillations in the atmospheric sector. Based on this result new limits on the mixing parameters of a massive sterile neutrino may be set. Preliminary results of the…

High Energy Physics - Experiment · Physics 2015-10-15 Luca Stanco

The MINOS long baseline neutrino oscillation experiment is comprised of three calorimeters, a Near Detector at FNAL, a Far Detector at the Soudan mine in northern Minnesota, and a Calibration Detector in a test beam at CERN. The light…

High Energy Physics - Experiment · Physics 2007-05-23 M. A. Barker , A. De Santo , P. Dervan , K. Lang , P. S. Miyagawa , R. Saakyan , S. Smith , D. Michael , J. Thomas , A. Weber

Searches for mass-3 component in the electron neutrino flavor state $\sin{\theta}_{13}$ and for sterile neutrinos can be carried out in the same small mixing angle antineutrino oscillation experiment at a reactor. As an example we consider…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. Kopeikin , L. Mikaelyan , V. Sinev

We review the current-generation short-baseline reactor neutrino experiments that have firmly established the third neutrino mixing angle $\theta_{13}$ to be non-zero. The relative large value of $\theta_{13}$ (around 9$^\circ$) has opened…

High Energy Physics - Experiment · Physics 2014-05-29 X. Qian , W. Wang

Precise tests of Lorentz invariance in neutrinos can be performed using long baseline experiments such as MINOS and OPERA or neutrinos from astrophysical sources. The MINOS collaboration reported a measurement of the muonic neutrino…

High Energy Physics - Phenomenology · Physics 2015-05-30 Giacomo Cacciapaglia , Aldo Deandrea , Luca Panizzi

A Neutrino Factory producing an intense beam composed of nu_e(nubar_e) and nubar_mu(nu_mu) from muon decays has been shown to have the greatest sensitivity to the two currently unmeasured neutrino mixing parameters, theta_13 and delta_CP .…

High Energy Physics - Experiment · Physics 2015-03-13 A. Cervera , A. Laing , J. Martin-Albo , F. J. P. Soler

A description is given of the light-injection calibration system that has been developed for the MINOS long-baseline neutrino oscillation experiment. The system is based upon pulsed blue LEDs monitored by PIN photodiodes. It is designed to…

The MINOS Collaboration continues its search for $\nu_e$ appearance in the NuMI (Neutrinos at the Main Injector) beam at Fermilab. Neutrinos in the beam interact in the Near Detector, located 1 km from the beam source, allowing us to…

High Energy Physics - Experiment · Physics 2015-03-19 Mhair Orchanian

We searched for a sidereal modulation in the rate of neutrinos produced by the NuMI beam and observed by the MINOS far detector. The detection of such harmonic signals could be a signature of neutrino-antineutrino mixing due to Lorentz and…

High Energy Physics - Experiment · Physics 2015-06-12 B. Rebel , S. Mufson

Neutrinos are elementary particles in the standard model of particle physics. There are 3 flavors of neutrinos that oscillate among themselves. Their oscillation can be described by a 3$\times$3 unitary matrix, containing three mixing…

High Energy Physics - Experiment · Physics 2015-06-19 Haoqi Lu

Neutrino physics is nowadays receiving more and more attention as a possible source of information for the long standing problem of new Physics beyond the Standard Model. The recent measurements of the third mixing angle $\theta_{13}$ in…

High Energy Physics - Phenomenology · Physics 2013-10-08 Luca Stanco , Stefano Dusini , Andrea Longhin , Alessandro Bertolin , Marco Laveder

This talk presented the first muon anti-neutrino disappearance analysis using data from the T2K anti-neutrino data taken in 2014 and up to March 12, 2015. The preliminary measured oscillation parameters, using $2.3\times 10^{20}$ protons on…

High Energy Physics - Experiment · Physics 2015-09-30 Blair Jamieson

We have investigated the possibility of discerning mass from flavor changing neutrino interactions induced $\nu_\mu \to \nu_\tau$ oscillations in the long baseline neutrino experiments K2K and MINOS. We have found that for virtually any…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. M. Gago , L. P. Freitas , O. L. G. Peres , R. Zukanovich Funchal

The MiniBooNE experiment has observed a significant excess of electron neutrinos in a muon neutrino beam at source-detector distances too short to be compatible with standard neutrino oscillations. The most straightforward explanation for…

High Energy Physics - Phenomenology · Physics 2020-07-01 Mona Dentler , Ivan Esteban , Joachim Kopp , Pedro Machado

New generation of three reactor neutrino experiments have made definitive measurements of the smallest neutrino mixing angle theta13 in 2012, based on the disappearance of electron antineutrinos. More precise measurements of the mixing…

High Energy Physics - Phenomenology · Physics 2015-05-01 Soo-Bong Kim

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

In the light of recent neutrino oscillation and non-oscillation data, we revisit the phenomenological constraints applicable to three observables sensitive to absolute neutrino masses: The effective neutrino mass in single beta decay…

High Energy Physics - Phenomenology · Physics 2008-11-26 G. L. Fogli , E. Lisi , A. Marrone , A. Melchiorri , A. Palazzo , P. Serra , J. Silk , A. Slosar