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Fermilab has had a very active long baseline neutrino program since initiation of the NuMI project in 1998. Commissioned in 2005, the NuMI beam with 400 kW design power has been in operation for the MINOS neutrino oscillation program since…

Accelerator Physics · Physics 2015-06-15 S. Childress , J. Strait

The Neutrinos at the Main Injector (NuMI) beamline will deliver an intense muon neutrino beam by focusing a beam of mesons into a long evacuated decay volume. The beam must be steered with 1 mRad angular accuracy toward the Soudan…

New physics beyond the Standard Model can lead to extra matter effects on neutrino oscillation if the new interactions distinguish among the three flavors of neutrino. In Ref.1, we argued that a long-baseline neutrino oscillation experiment…

High Energy Physics - Phenomenology · Physics 2017-08-23 Minako Honda , Yee Kao , Naotoshi Okamura , Alexey Pronin , Tatsu Takeuchi

A muon collider is expected to produce a high intensity neutrino beam which is an admixture of either $\nu_{\mu}+\bar{\nu_e}$ or $\bar{\nu}_{\mu} +\nu_e$ which can can be directed to underground detectors far away from the source. It will…

High Energy Physics - Phenomenology · Physics 2011-07-19 R. N. Mohapatra

The neutrinos from a Type II supernova provide perhaps our best opportunity to probe cosmologically interesting muon and/or tauon neutrino masses. This is because matter enhanced neutrino oscillations can lead to an anomalously hot nu_e…

Astrophysics · Physics 2010-12-02 G. M. Fuller , W. C. Haxton , G. C. McLaughlin

One phenomenological explanation of superluminal propagation of neutrinos, which may have been observed by OPERA and MINOS, is that neutrinos travel faster inside of matter than in vacuum. If so neutrinos exhibit refraction inside matter…

High Energy Physics - Experiment · Physics 2011-10-13 Albert Stebbins

The NO$\nu$A experiment is a long-baseline accelerator based neutrino oscillation experiment. It uses the upgraded Fermilab NuMI beam and measures electron-neutrino appearance and muon-neutrino disappearance at its far detector in Ash…

Instrumentation and Detectors · Physics 2013-10-01 Jianming Bian

We suggest that the presence of a quantum gravity induced minimal length can be explored using neutrino oscillation probabilities. Neutrinos seem ideally suited for this investigation because they can propagate freely over large distances…

High Energy Physics - Phenomenology · Physics 2011-11-21 Martin Sprenger , Piero Nicolini , Marcus Bleicher

MuOn-decay MEdium baseline NeuTrino beam experiment (MOMENT) is a next-generation accelerator neutrino experiment looking for more physics study. We try to simulate neutrino oscillations confronting with Charged-Current\&Non-Standard…

High Energy Physics - Phenomenology · Physics 2018-03-02 Jian Tang , Yibing Zhang

The recent discovery that neutrinos have mass opens a wide new field of experimentation. Accelerator-made neutrinos are essential. Ideas for future facilities include superbeams beta-beams and neutrino factories, each associated with one or…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alain Blondel

We show that a breakdown of the universality of the gravitational couplings to different neutrino flavors can be tested in long-baseline neutrino-oscillation experiments. In particular we have analyzed in detail a proposed experiment at…

High Energy Physics - Phenomenology · Physics 2015-06-25 Kazuhito Iida , Hisakazu Minakata , Osamu Yasuda

In this paper I give an overview of the status of neutrino oscillation experiments performed using nuclear reactors as sources of neutrinos. I review the present generation of experiments (Chooz and Palo Verde) with baselines of about 1 km…

High Energy Physics - Experiment · Physics 2009-10-31 Giorgio Gratta

The weak interactions of neutrinos with other Standard Model particles are well described within the Standard Model of particle physics. However, modern accelerator-based neutrino experiments employ nuclei as targets, where neutrinos…

High Energy Physics - Phenomenology · Physics 2025-11-10 Vishvas Pandey

The planned neutrino program at Fermilab requires large proton beam intensities in excess of 2 MW. Measuring the transverse profiles of these high intensity beams is challenging and often depends on non-invasive techniques. One such…

Accelerator Physics · Physics 2018-03-06 R. Thurman-Keup , M. Alvarez , J. Fitzgerald , C. Lundberg , P. Prieto , J. Zagel , W. Blokland

New physics beyond the Standard Model can lead to extra matter effects on neutrino oscillation if the new interactions distinguish among the three flavors of neutrino. In a previous paper, we argued that a long-baseline neutrino oscillation…

High Energy Physics - Phenomenology · Physics 2007-08-07 Minako Honda , Yee Kao , Naotoshi Okamura , Alexey Pronin , Tatsu Takeuchi

We investigate the possible production of a MeV-scale sterile fermion through the up-scattering of neutrinos on nuclei and atomic electrons at different facilities. We consider a phenomenological model that adds a new fermion to the…

High Energy Physics - Phenomenology · Physics 2024-11-20 Pablo M. Candela , Valentina De Romeri , Pantelis Melas , Dimitrios K. Papoulias , Niki Saoulidou

Spectacular processes in astrophysical sites produce high-energy cosmic rays which are further accelerated by Fermi-shocks into a power-law spectrum. These, in passing through radiation fields and matter, produce neutrinos. Neutrino…

High Energy Physics - Phenomenology · Physics 2010-12-03 Ivone F. M. Albuquerque , Jodi Lamoureux , George F. Smoot

The Spallation Neutron Source (SNS), located at Oak Ridge Laboratory in the United States, will be coming online over the next few years. In addition to producing fluxes of high-intensity neutrons, the interaction of the proton beam with…

High Energy Physics - Experiment · Physics 2019-08-13 Heather Ray

The NOvA long-baseline neutrino experiment uses a pair of large, segmented, liquid-scintillator calorimeters to study neutrino oscillations, using GeV-scale neutrinos from the Fermilab NuMI beam. These detectors are also sensitive to the…

Instrumentation and Detectors · Physics 2023-02-18 NOvA Collaboration , M. A. Acero , P. Adamson , G. Agam , L. Aliaga , T. Alion , V. Allakhverdian , N. Anfimov , A. Antoshkin , E. Arrieta-Diaz , L. Asquith , A. Aurisano , A. Back , C. Backhouse , M. Baird , N. Balashov , P. Baldi , B. A. Bambah , S. Bashar , K. Bays , S. Bending , R. Bernstein , V. Bhatnagar , B. Bhuyan , J. Bian , J. Blair , A. C. Booth , P. Bour , R. Bowles , C. Bromberg , N. Buchanan , A. Butkevich , V. Bychkov , S. Calvez , T. J. Carroll , E. Catano-Mur , S. Childress , B. C. Choudhary , T. E. Coan , M. Colo , L. Corwin , L. Cremonesi , G. S. Davies , P. F. Derwent , P. Ding , Z. Djurcic , M. Dolce , D. Doyle , D. Dueñas Tonguino , E. C. Dukes , P. Dung , H. Duyang , S. Edayath , R. Ehrlich , M. Elkins , G. J. Feldman , P. Filip , W. Flanagan , J. Franc , M. J. Frank , H. R. Gallagher , R. Gandrajula , F. Gao , S. Germani , A. Giri , R. A. Gomes , M. C. Goodman , V. Grichine , M. Groh , R. Group , B. Guo , A. Habig , F. Hakl , A. Hall , J. Hartnell , R. Hatcher , A. Hatzikoutelis , K. Heller , V Hewes , A. Himmel , A. Holin , B. Howard , J. Huang , J. Hylen , F. Jediny , C. Johnson , M. Judah , I. Kakorin , D. Kalra , D. M. Kaplan , R. Keloth , O. Klimov , L. W. Koerner , L. Kolupaeva , S. Kotelnikov , M. Kubu , Ch. Kullenberg , A. Kumar , C. D. Kuruppu , V. Kus , T. Lackey , K. Lang , L. Li , S. Lin , A. Lister , M. Lokajicek , S. Luchuk , S. Magill , W. A. Mann , M. L. Marshak , M. Martinez-Casales , V. Matveev , B. Mayes , D. P. Méndez , M. D. Messier , H. Meyer , T. Miao , W. H. Miller , S. R. Mishra , A. Mislivec , R. Mohanta , A. Moren , A. Morozova , L. Mualem , M. Muether , S. Mufson , K. Mulder , R. Murphy , J. Musser , D. Naples , N. Nayak , J. K. Nelson , R. Nichol , G. Nikseresht , E. Niner , A. Norman , A. Norrick , T. Nosek , A. Olshevskiy , T. Olson , J. Paley , R. B. Patterson , G. Pawloski , O. Petrova , R. Petti , R. K. Plunkett , F. Psihas , A. Rafique , V. Raj , B. Ramson , B. Rebel , P. Rojas , V. Ryabov , O. Samoylov , M. C. Sanchez , S. Sánchez Falero , I. S. Seong , P. Shanahan , A. Sheshukov , P. Singh , V. Singh , E. Smith , J. Smolik , P. Snopok , N. Solomey , A. Sousa , K. Soustruznik , M. Strait , L. Suter , A. Sutton , C. Sweeney , R. L. Talaga , B. Tapia Oregui , P. Tas , R. B. Thayyullathil , J. Thomas , E. Tiras , D. Torbunov , J. Tripathi , A. Tsaris , Y. Torun , J. Urheim , P. Vahle , Z. Vallari , J. Vasel , P. Vokac , T. Vrba , M. Wallbank , T. K. Warburton , M. Wetstein , D. Whittington , D. A. Wickremasinghe , S. G. Wojcicki , J. Wolcott , A. Yallappa Dombara , K. Yonehara , S. Yu , Y. Yu , S. Zadorozhnyy , J. Zalesak , Y. Zhang , R. Zwaska

Future neutrino oscillation experiments will lead to precision measurements of neutrino mass splittings and mixings. The flavour structure of the lepton sector will therefore at some point become better known than that of the quark sector.…

High Energy Physics - Phenomenology · Physics 2014-11-18 Manfred Lindner
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