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Related papers: On the Optimum Long Baseline for the Next Generati…

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For standard interactions of neutrinos with matter bimagic baseline of length about 2540 Km is known to be suitable for getting good discovery limits of neutrino mass hierarchy, $\sin^2 \theta_{13}$ and CP violation in the $\nu_e…

High Energy Physics - Phenomenology · Physics 2012-04-10 Rathin Adhikari , Arnab Dasgupta , Zini Rahman

ESS$\nu$SB is a proposed neutrino super-beam project at the ESS facility. We study the performance of this setup in the presence of a light eV-scale sterile neutrino, considering 540 km baseline with 2 years (8 years) of $\nu$ ($\bar\nu$)…

High Energy Physics - Phenomenology · Physics 2020-01-29 Sanjib Kumar Agarwalla , Sabya Sachi Chatterjee , Antonio Palazzo

Future long baseline neutrino experiments such as the DUNE experiment under construction at Fermilab will perform precision measurements of neutrino oscillations, including the potential for the discovery of CP violation in the lepton…

Instrumentation and Detectors · Physics 2019-05-22 Lorenz Emberger , Frank Simon

In this paper we quantify the trade-off between setups optimized to be ancillary to Phase II Superbeams or Neutrino Factories and experiments tuned for maximal sensitivity to the subdominant terms of the neutrino transition probability at…

High Energy Physics - Phenomenology · Physics 2009-11-10 P. Migliozzi , F. Terranova

This is a report on recent progress and developments since the NANP'99 Conference in current and future long baseline (~1 km) and very long baseline (~100 - 800 km) oscillation experiments at reactors. These experiments, under certain…

High Energy Physics - Experiment · Physics 2007-05-23 L. Mikaelyan

This report provides the results of an extensive and important study of the potential for a U.S. scientific program that will extend our knowledge of neutrino oscillations well beyond what can be anticipated from ongoing and planned…

I give a brief overview of the physics potential of short baseline experiments at neutrino factories, i.e. facilities providing high energy and high intensity neutrino beams, like the one planned to be built in connection with the proposed…

High Energy Physics - Phenomenology · Physics 2009-10-31 Alexey A. Petrov

We explore the physics reach of several possible configurations for a Super-Beam experiment in Europe, focusing on the possibilities of discovering $\theta_{13}$, CP violation in the leptonic sector and the ordering of neutrino mass…

High Energy Physics - Phenomenology · Physics 2011-10-13 Pilar Coloma , Tracey Li , Silvia Pascoli

We discuss in detail the physics reach of an experimental set-up where electron neutrinos (anti-neutrinos) produced in a beta-beam facility at Fermi National Accelerator Laboratory (FNAL) are sent, over a distance of L~1300km, to the Deep…

High Energy Physics - Phenomenology · Physics 2015-03-13 Sanjib Kumar Agarwalla , Patrick Huber

The MINOS long baseline experiment has been collecting neutrino beam data since March 2005 and has accumulated 3 x 10^{20} protons-on-target (POT) to date. MINOS uses Fermilab's NuMI neutrino beam which is measured by two steel-scintillator…

High Energy Physics - Experiment · Physics 2007-06-13 Tobias M. Raufer

Neutrino Factory is a facility for future precision studies of neutrino oscillations. A so called near detector is essential for reaching the aimed precision of neutrino oscillation analysis. Main task of the near detector is to measure the…

High Energy Physics - Experiment · Physics 2011-10-11 Rosen Matev , Roumen Tsenov

Recent measurements by the T2K neutrino oscillation experiment indicate that CP violation in neutrino mixing may be observed in the future by long-baseline neutrino oscillation experiments. We propose an extension to the currently approved…

High Energy Physics - Experiment · Physics 2016-09-15 K. Abe , H. Aihara , A. Amji , J. Amey , C. Andreopoulos , M. Antonova , S. Aoki , A. Atherton , S. Ban , F. C. T. Barbato , M. Barbi , F. C. T. Barbato , G. J. Barker , G. Barr , P. Bartet-Friburg , M. Batkiewicz , V. Berardi , S. Bhadra , S. Bienstock , A. Blondel , S. Bolognesi , S. Bordoni , S. B. Boyd , D. Brailsford , A. Bravar , C. Bronner , M. Buizza Avanzini , J. Calcutt , R. G. Calland , D. Calvet , T. Campbell , S. Cao , S. L. Cartwright , R. Castillo , M. G. Catanesi , A. Cervera , C. Checchia , D. Cherdack , N. Chikuma , G. Christodoulou , A. Clifton , J. Coleman , G. Collazuol , D. Coplowe , L. Cremonesi , A. Cudd , A. Dabrowska , A. Delbart , G. De Rosa , T. Dealtry , P. F. Denner , S. R. Dennis , C. Densham , D. Dewhurst , F. Di Lodovico , S. Dolan , O. Drapier , K. E. Duffy , J. Dumarchez , M. Dunkman , M. Dziewiecki , S. Emery-Schrenk , P. Fernanddez , T. Feusels , A. J. Finch , G. A. Fiorentini , G. Fiorillo , M. Fitton , M. Friend , Y. Fujii , D. Fukuda , Y. Fukuda , A. Garcia , C. Giganti , F. Gizzarelli , M. Gonin , N. Grant , D. R. Hadley , L. Haegel , M. D. Haigh , D. Hansen , J. Harada , M. Hartz , T. Hasegawa , N. C. Hastings , T. Hayashino , Y. Hayato , T. Hiraki , A. Hiramoto , S. Hirota , M. Hogan , J. Holeczek , F. Hosomi , K. Huang , A. K. Ichikawa , M. Ikeda , J. Imber , J. Insler , R. A. Intonti , T. Ishida , T. Ishii , E. Iwai , K. Iwamoto , A. Izmaylov , B. Jamieson , M. Jiang , S. Johnson , J. H. Jo , P. Jonsson , C. K. Jung , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , T. Katori , E. Kearns , M. Khabibullin , A. Khotjantsev , H. Kim , S. King , J. Kisiel , A. Knight , A. Knox , T. Kobayashi , L. Koch , T. Koga , A. Konaka , K. Kondo , L. L. Kormos , A. Korzenev , Y. Koshio , K. L. Kowalik , W. Kropp , Y. Kudenko , R. Kurjata , T. Kutter , L. Labarga , J. Lagoda , I. Lamont , M. Lamoureux , E. Larkin , P. Lasorak , M. Laveder , M. Lawe , T. Lindner , Z. J. Liptak , R. P. Litchfield , X. Li , A. Longhin , J. P. Lopez , T. Lou , L. Ludovici , X. Lu , L. Magaletti , K. Mahn , M. Malek , S. Manly , A. D. Marino , J. F. Martin , P. Martins , S. Martynenko , T. Maruyama , V. Matveev , K. Mavrokoridis , W. Y. Ma , E. Mazzucato , M. McCarthy , N. McCauley , K. S. McFarland , C. McGrew , A. Mefodiev , C. Metelko , M. Mezzetto , P. Mijakowski , A. Minamino , O. Mineev , S. Mine , A. Missert , M. Miura , S. Moriyama , Th. A. Mueller , Y. Nagai , T. Nakadaira , M. Nakahata , K. G. Nakamura , K. Nakamura , K. D. Nakamura , Y. Nakanishi , S. Nakayama , T. Nakaya , K. Nakayoshi , C. Nantais , K. Nishikawa , Y. Nishimura , P. Novella , J. Nowak , H. M. O'Keeffe , R. Ohta , K. Okumura , T. Okusawa , T. Ovsyannikova , R. A. Owen , Y. Oyama , V. Palladino , J. L. Palomino , V. Paolone , W. Parker , N. D. Patel , M. Pavin , D. Payne , J. D. Perkin , L. Pickard , L. Pickering , E. S. Pinzon Guerra , B. Popov , M. Posiadala-Zezula , J. -M. Poutissou , R. Poutissou , P. Przewlocki , B. Quilain , T. Radermacher , E. Radicioni , P. N. Ratoff , M. Ravonel , M. A. Rayner , E. Reinherz-Aronis , C. Riccio , P. Rojas , E. Rondio , B. Rossi , S. Roth , A. C. Ruggeri , A. Rychter , R. Sacco , K. Sakashita , F. Sánchez , E. Scantamburlo , K. Scholberg , J. Schwehr , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , R. Shah , A. Shaikhiev , F. Shaker , D. Shaw , M. Shiozawa , T. Shirahige , S. Short , M. Smy , J. T. Sobczyk , H. Sobel , L. Southwell , J. Steinmann , T. Stewart , P. Stowell , Y. Suda , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , M. Szeptycka , R. Tacik , M. Tada , A. Takeda , Y. Takeuchi , R. Tamura , H. K. Tanaka , H. A. Tanaka , D. Terhorst , R. Terri , T. Thakore , L. F. Thompson , W. Toki , T. Tomura , C. Touramanis , T. Tsukamoto , M. Tzanov , M. A. Uchida , Y. Uchida , M. Vagins , A. Vacheret , Z. Vallari , G. Vasseur , T. Wachala , C. W. Walter , D. Wark , M. O. Wascko , A. Weber , R. Wendell , R. J. Wilkes , M. J. Wilking , J. R. Wilson , R. J. Wilson , C. Wret , Y. Yamada , K. Yamamoto , M. Yamamoto , C. Yanagisawa , T. Yano , S. Yen , N. Yershov , M. Yokoyama , J. Yoo , K. Yoshida , T. Yuan , M. Yu , A. Zalewska , J. Zalipska , L. Zambelli , K. Zaremba , M. Ziembicki , E. D. Zimmerman , M. Zito

The feasibility study of an underground laboratory in the Polkowice -Sieroszowice mine in Poland (SUNLAB) as a host of a far detector in a long-baseline neutrino oscillation experiment was performed. The SUNLAB location was previously…

High Energy Physics - Phenomenology · Physics 2019-07-24 Malgorzata Haranczyk

We propose a $\beta$-Beam experiment with four source ions and two baselines for the best possible sensitivity to $\theta_{13}$, CP violation and mass hierarchy. Neutrinos from $^{18}$Ne and $^6$He with Lorentz boost $\gamma=350$ are…

High Energy Physics - Phenomenology · Physics 2010-05-07 Pilar Coloma

The standard three-neutrino oscillation paradigm, associated with small squared mass splittings $\ll 0.1\ \mathrm{eV^2}$, has been successfully built up over the last 15 years using solar, atmospheric, long baseline accelerator and reactor…

Instrumentation and Detectors · Physics 2015-04-16 J. Gaffiot , T. Lasserre , G. Mention , M. Vivier , M. Cribier , M. Durero , V. Fischer , A. Letourneau , E. Dumonteil , I. S. Saldikov , G. V. Tikhomirov

The ESS$\nu$SB project proposes to base a neutrino ''Super Beam'' of unprecedented luminosity at the European Spallation Source. The original proposal identified the second peak of the oscillation probability as the optimal to maximize the…

High Energy Physics - Phenomenology · Physics 2020-09-15 M. Blennow , E. Fernandez-Martinez , T. Ota , S. Rosauro-Alcaraz

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

Neutrino oscillation among the three active neutrino flavors is well established and supported by experiments at diverse length scales and energy scales. It may be noted that five of the neutrino oscillation parameters in the three-flavor…

High Energy Physics - Phenomenology · Physics 2026-01-13 Rajrupa Banerjee , Jogesh Rout , Sudhanwa Patra , Poonam Mehta

Experiments strongly suggest that the flavour mixing responsible for the atmospheric neutrino anomaly is very close to being maximal. Thus, it is of great theoretical as well as experimental importance to measure any possible deviation from…

High Energy Physics - Phenomenology · Physics 2009-11-10 Debajyoti Choudhury , Anindya Datta

LBNE (Longbaseline Neutrino Oscillation Experiments) provide a powerful experimental setup to study sensitivities and exlcusion limits in neutrino oscillation parameter space. A longbaseline experiment is being planned, at USA, from FNAL…

High Energy Physics - Phenomenology · Physics 2014-06-24 Kalpana Bora