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Beta Beams could address the needs of long term neutrino oscillation experiments. They can produce extremely pure neutrino beams through the decays of relativistic radioactive ions. The baseline scenario is described, together with its…

High Energy Physics - Experiment · Physics 2009-11-10 M. Mezzetto

The two-detector design of the NOvA neutrino oscillation experiment, in which two functionally identical detectors are exposed to an intense neutrino beam, aids in canceling leading order effects of cross-section uncertainties. However,…

High Energy Physics - Experiment · Physics 2023-02-18 NOvA Collaboration , M. A. Acero , P. Adamson , G. Agam , L. Aliaga , T. Alion , V. Allakhverdian , N. Anfimov , A. Antoshkin , 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 , 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 , D. Doyle , 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 , 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 , Ch. Kullenberg , A. Kumar , C. D. Kuruppu , V. Kus , T. Lackey , K. Lang , L. Li , S. Lin , M. Lokajicek , S. Luchuk , K. Maan , 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 , A. Rafique , F. Psihas , A. Radovic , 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 , Y. Torun , J. Urheim , P. Vahle , Z. Vallari , J. Vasel , P. Vokac , T. Vrba , M. Wallbank , T. K. Warburton , M. Wetstein , D. Whittington , S. G. Wojcicki , J. Wolcott , A. Yallappa Dombara , K. Yonehara , S. Yu , Y. Yu , S. Zadorozhnyy , J. Zalesak , Y. Zhang , R. Zwaska

Neutrino beams at from high-energy proton accelerators have been instrumental discovery tools in particle physics. Neutrino beams are derived from the decays of charged pi and K mesons, which in turn are created from proton beams striking…

Accelerator Physics · Physics 2008-11-26 Sacha E. Kopp

Recently we have proposed a new concept of a thermal neutron detector based on resistive plate chambers and 10B4C solid neutron converters, enabling to readout with high resolution in both the 3D position of neutron capture and the neutron…

We review detector technologies which are currently considered for ultimate nucleon decay searches, new generation astrophysical neutrinos studies, and for future long-baseline neutrino experiments at new high-intensity neutrino beam…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Rubbia

NOvA is a long-baseline neutrino experiment that uses an upgraded NuMI neutrino source at Fermilab and a 14-kton detector at Ash River, Minnesota. The detector has a highly active, finely segmented design that offers superb event…

High Energy Physics - Experiment · Physics 2018-12-27 Jianming Bian

MINERvA (Main INjector ExpeRiment v-A) is a few-GeV neutrino scattering experiment that began taking data in the NuMI beam at Fermilab (FNAL) in the Fall of 2009. MINERvA employs a fine-grained detector, with an eight ton active target…

High Energy Physics - Experiment · Physics 2019-08-13 Gabriel N. Perdue

Knowledge of the neutrino flux produced by the Neutrinos at the Main Injector (NuMI) beamline is essential to the neutrino oscillation and neutrino interaction measurements of the MINERvA, MINOS+, NOvA and MicroBooNE experiments at Fermi…

Neutrino beam with about 300 MeV in energy, high-flux and medium baseline is considered a rational choice for measuring CP violation before the more powerful Neutrino Factory will be built. Following this concept, a unique neutrino beam…

Controlling non-linear effects in the transverse dynamics of charged particle beams in circular accelerators opens new possibilities for controlling some of the beam properties. Beam splitting by crossing a stable 1D non-linear resonance is…

Accelerator Physics · Physics 2022-02-10 A. Bazzani , F. Capoani , M. Giovannozzi

The long-term prospects for fully exploring three-flavor mixing in the neutrino sector depend upon an ongoing and increased investment in the appropriate accelerator R&D. Two new concepts have been proposed that would revolutionize neutrino…

A problem of vibration control of smart beams was addressed in various publications which primarily utilize collocated sensors and actuators and neglect the effect of measurement noise in the observer design. This paper develops a natural…

Optimization and Control · Mathematics 2014-10-30 M. A. Pinsky , A. O. Ozer

NOvA is a long-baseline neutrino oscillation experiment that detects neutrino particles from the NuMI beam at Fermilab. Before data from this experiment can be used in analyses, raw hits in the detector must be matched to their source…

Machine Learning · Computer Science 2025-11-13 Edgar E. Robles , Dikshant Sagar , Alejandro Yankelevich , Jianming Bian , Pierre Baldi , NOvA Collaboration

In recent years great progress toward the understanding of the mixing in the leptonic sector has been made. Nonetheless, this field of research is just at the beginning. Further advance by accelerator based neutrino oscillation experiments…

High Energy Physics - Phenomenology · Physics 2007-05-23 Pasquale Migliozzi

NOvA is a long-baseline neutrino oscillation experiment. It is optimized to measure $\nu_e$ appearance and $\nu_{\mu}$ disappearance at the Far Detector in the $\nu_{\mu}$ beam produced by the NuMI facility at Fermilab. NOvA uses a…

Instrumentation and Detectors · Physics 2019-10-30 Shiqi Yu

In nuclear and atomic physics experiments, charged ion beams often need to be guided from the ion production to the experimental site. In the PUMA experiment, an ion source beamline was developed, which can be operated with up to…

We describe a procedure for engineering beams of cold atoms by selectively draining particles from a trapped gas based on momenta. Atoms escape through a filter potential that only transmits atoms with the desired momenta. We outline an…

Quantum Gases · Physics 2019-09-10 D Hudson Smith , Artem G Volosniev

Standard three-flavor neutrino oscillations have well explained by a wide range of neutrino experiments. However, the anomalous results, such as electron-antineutrino excess seen by LSND and MiniBooNE do not fit the three-flavor paradigm.…

High Energy Physics - Experiment · Physics 2017-10-03 Rijeesh Keloth , Adam Aurisano , Alexander Sousa , Gavin S Davies , Louise Suter , Robert K Plunkett

A new strategy is proposed to control interior permanent magnet generators in dc microgrids interfaced through an active rectifier. The controller design is based on the decomposition of the system dynamics into slow and fast modes using…

Systems and Control · Electrical Eng. & Systems 2020-10-09 Luis Herrera , Chad Miller , Bang-Hung Tsao

The physics goals of NOvA are the constraints of neutrino oscillation parameters such as the octant of $\theta_{23}$, $\delta_{\rm{CP}}$, and the neutrino mass hierarchy via a joint fit to $\nu_{\mu}$ and $\nu_{e}$ oscillation spectrum. We…

High Energy Physics - Experiment · Physics 2018-09-03 Reddy Pratap Gandrajula , Micah Groh