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Related papers: Combining CPT-conjugate Neutrino channels at Fermi…

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We discuss the capabilities of a future neutrino factory based on intense neutrino beams from a muon storage ring to explore the non-standard neutrino matter interactions, which are assumed to be sub-leading effects in the standard mass…

High Energy Physics - Phenomenology · Physics 2014-11-17 A. M. Gago , M. M. Guzzo , H. Nunokawa , W. J. C. Teves , R. Zukanovich Funchal

Beams of neutrinos have been proposed as a vehicle for communications under unusual circumstances, such as direct point-to-point global communication, communication with submarines, secure communications and interstellar communication. We…

High Energy Physics - Experiment · Physics 2012-04-10 D. D. Stancil , P. Adamson , M. Alania , L. Aliaga , M. Andrews , C. Araujo Del Castillo , L. Bagby , J. L. Bazo Alba , A. Bodek , D. Boehnlein , R. Bradford , W. K. Brooks , H. Budd , A. Butkevich , D. A. M. Caicedo , D. P. Capista , C. M. Castromonte , A. Chamorro , E. Charlton , M. E. Christy , J. Chvojka , P. D. Conrow , I. Danko , M. Day , J. Devan , J. M. Downey , S. A. Dytman , B. Eberly , J. R. Fein , J. Felix , L. Fields , G. A. Fiorentini , A. M. Gago , H. Gallagher , R. Gran , J. Grange , J. Griffin , T. Griffin , E. Hahn , D. A. Harris , A. Higuera , J. A. Hobbs , C. M. Hoffman , B. L. Hughes , K. Hurtado , A. Judd , T. Kafka , K. Kephart , J. Kilmer , M. Kordosky , S. A. Kulagin , V. A. Kuznetsov , M. Lanari , T. Le , H. Lee , L. Loiacono , G. Maggi , E. Maher , S. Manly , W. A. Mann , C. M. Marshall , K. S. McFarland , A. Mislivec , A. M. McGowan , J. G. Morfin , H. da Motta , J. Mousseau , J. K. Nelson , J. A. Niemiec-Gielata , N. Ochoa , B. Osmanov , J. Osta , J. L. Palomino , J. S. Paradis , V. Paolone , J. Park , C. Pena , G. Perdue , C. E. Perez Lara , A. M. Peterman , A. Pla-Dalmau , B. Pollock , F. Prokoshin , R. D. Ransome , H. Ray , M. Reyhan , P. Rubinov , D. Ruggiero , O. S. Sands , H. Schellman , D. W. Schmitz , E. C. Schulte , C. Simon , C. J. Solano Salinas , R. Stefanski , R. G. Stevens , N. Tagg , V. Takhistov , B. G. Tice , R. N. Tilden , J. P. Velasquez , I. Vergalosova , J. Voirin , J. Walding , B. J. Walker , T. Walton , J. Wolcott , T. P. Wytock , G. Zavala , D. Zhang , L. Y. Zhu , B. P. Ziemer

Up to now, future neutrino beam experiments have been designed and optimized in order to look for CP violation, \theta_{13} and the mass hierarchy under the conservative assumption that \theta_{13} is very small. However, the recent results…

High Energy Physics - Phenomenology · Physics 2015-05-30 Pilar Coloma , Enrique Fernandez-Martinez

We adopt a bottom-up approach to reconstruct the possible neutrino mass matrix patterns, in the hypothesis that $\lambda = \sin \theta_C$, where $\theta_C$ is the Cabibbo angle, is a useful expansion parameter in the neutrino sector as it…

High Energy Physics - Phenomenology · Physics 2010-09-14 Fu-Sin Ling

The nuSTORM facility has been designed to deliver beams of electron neutrinos and muon neutrinos (and their anti-particles) from the decay of a stored muon beam with a central momentum of 3.8 GeV/c and a momentum acceptance of 10%. The…

Accelerator Physics · Physics 2017-03-20 D. Adey , S. K. Agarwalla , C. M. Ankenbrandt , R. Asfandiyarov , J. J. Back , G. Barker , E. Baussan , R. Bayes , S. Bhadra , V. Blackmore , A. Blondel , S. A. Bogacz , C. Booth , S. B. Boyd , A. Bravar , S. J. Brice , A. D. Bross , F. Cadoux , H. Cease , A. Cervera , J. Cobb , D. Colling , P. Coloma , L. Coney , A. Dobbs , J. Dobson , A. Donini , P. Dornan , M. Dracos , F. Dufour , R. Edgecock , J. Evans , M. Geelhoed , M. A. George , T. Ghosh , J. J. Gomez-Cadenas , A. de Gouvea , A. Haesler , G. Hanson , P. F. Harrison , M. Hartz , P. Hernandez , J. A. Hernando Morata , P. Hodgson , P. Huber , A. Izmaylov , Y. Karadzhov , T. Kobilarcik , J. Kopp , L. Kormos , A. Korzenev , Y. Kuno , A. Kurup , P. Kyberd , J. B. Lagrange , A. Laing , A. Liu , J. M. Link , K. Long , K. Mahn , C. Mariani , C. Martin , J. Martin , N. McCauley , K. T. McDonald , O. Mena , S. R. Mishra , N. Mokhov , J. Morfin , Y. Mori , W. Murray , D. Neuffer , R. Nichol , E. Noah , M. A. Palmer , S. Parke , S. Pascoli , J. Pasternak , M. Popovic , P. Ratoff , M. Ravonel , M. Rayner , S. Ricciardi , C. Rogers , P. Rubinov , E. Santos , A. Sato , T. Sen , E. Scantamburlo , J. K. Sedgbeer , D. R. Smith , P. J. Smith , J. T. Sobczyk , L. Soby , F. J. P. Soler , S. Soldner-Rembold , M. Sorel , P. Snopok , P. Stamoulis , L. Stanco , S. Striganov , H. A. Tanaka , I. J. Taylor , C. Touramanis , C. D. Tunnell , Y. Uchida , N. Vassilopoulos , M. O. Wascko , A. Weber , M. J. Wilking , E. Wildner , W. Winter , U. K. Yang

The proposed PINGU experiment to measure the neutrino mass hierarchy is presented, in the context of long-range planning by the U.S. nuclear physics community.

Instrumentation and Detectors · Physics 2019-08-14 D. F. Cowen , T. DeYoung , D. Grant , D. A. Dwyer , S. R. Klein , K. B. Luk , D. R. Williams

In the first part of the present work the $\mu-\tau $ symmetry of the neutrino mass matrix is perturbed at its minimal level in order to produce deviation from Tri-bimaximal mixing (TBM), which includes nonzero value of reactor angle…

High Energy Physics - Phenomenology · Physics 2012-07-02 Subhankar Roy , N. Nimai Singh

In this proceedings we explore the physics potential of the ESSnuSBplus setup to study beam and non-beam based physics scenarios in both standard and new physics cases. The ESSnuSBplus setup consists of three neutrino sources: the main ESS…

High Energy Physics - Phenomenology · Physics 2026-01-16 ESSnuSB , : , Monojit Ghosh

The Neutrinos at the Main Injector (NuMI) beamline at Fermilab generates an intense muon neutrino beam for the NOvA (NuMI Off-axis $\nu_e$ Appearance) long-baseline neutrino experiment. Over the years, the NuMI beamline has been pivotal in…

Accelerator Physics · Physics 2024-12-18 D. A. A. Wickremasinghe , K. Yonehara

We investigate possible tests of CPT invariance on the level of event rates at neutrino factories. We do not assume any specific model but phenomenological differences in the neutrino-antineutrino masses and mixing angles in a Lorentz…

High Energy Physics - Phenomenology · Physics 2009-05-20 Samoil M. Bilenky , Martin Freund , Manfred Lindner , Tommy Ohlsson , Walter Winter

Recent measurements of large theta_{13} by Daya Bay and RENO reactor experiments have opened up the possibility of determining the neutrino mass hierarchy, i.e. the sign of the mass squared splitting Delta m_{31}^2, the CP-violating phase…

High Energy Physics - Phenomenology · Physics 2014-04-23 Rupak Dutta , Nita Sinha , Sushant K. Raut

The Neutrinos at the Main Injector (NuMI) facility at Fermilab began operations in late 2004. NuMI will deliver an intense muon neutrino beam of variable energy (2-20 GeV) directed into the Earth at 58 mrad for short (~1km) and long…

Accelerator Physics · Physics 2007-05-23 Sacha E. Kopp

ArgoNeuT, a Liquid Argon Time Projection Chamber (LAr-TPC), has collected thousands of neutrino and anti-neutrino events between 0.1 and 10 GeV in the NuMI beamline at Fermilab (FNAL). Among other issues, the experiment will measure the…

High Energy Physics - Experiment · Physics 2011-10-17 O. Palamara

Measuring the total neutrino mass is one of the most exciting opportunities available with next-generation cosmological data sets. We study the possibility of detecting the total neutrino mass using large-scale clustering in 21cm intensity…

Cosmology and Nongalactic Astrophysics · Physics 2022-01-19 Mario Ballardini , Roy Maartens

There are recent considerations to increase the photomultiplier density in the IceCube detector array beyond that of DeepCore, which will lead to a lower detection threshold and a huge fiducial mass for the neutrino detection. This…

High Energy Physics - Phenomenology · Physics 2015-05-30 Jian Tang , Walter Winter

The Long Baseline Neutrino Experiment (LBNE) will utilize a neutrino beamline facility located at Fermilab. The facility is designed to aim a beam of neutrinos toward a detector placed at the Deep Underground Science and Engineering…

In Fermilab's neutrino facilities such as the Neutrinos at the Main Injector (NuMI) and the upcoming Long Baseline Neutrino Facility (LBNF), a proton beam strikes high-power target, producing positively and negatively charged pions and…

Accelerator Physics · Physics 2024-01-24 D. A. Wickremasinghe , S. Ganguly , K. Yonehara , R. Zwaska , P. Snopok , Y. Yu

This article describes a new experimental method for accelerator based neutrino experiments called neutrino tagging. The method consists in exploiting the neutrino production mechanism, the $\pi^{\pm}\to\mu^{\pm}\nu_\mu$ decay, to…

High Energy Physics - Experiment · Physics 2022-06-02 Mathieu Perrin-Terrin

A search for neutral heavy leptons (NHLs) has been performed using an instrumented decay channel at the NuTeV (E-815) experiment at Fermilab. The decay channel was composed of helium bags interspersed with drift chambers, and was used in…

High Energy Physics - Experiment · Physics 2008-11-26 A. Vaitaitis

In this paper we consider a Beta Beam setup that tries to leverage at most existing European facilities: i.e. a setup that takes advantage of facilities at CERN to boost high-Q ions (8Li and 8B) aiming at a far detector located at L = 732…

High Energy Physics - Phenomenology · Physics 2015-05-18 P. Coloma , A. Donini , P. Migliozzi , L. Scotto Lavina , F. Terranova