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Related papers: Optimization of the Two-Baseline Beta-Beam

200 papers

We study the optimization of a green-field, two-baseline reactor experiment with respect to the sensitivity for electron antineutrino disappearance in search of a light sterile neutrino. We consider both commercial and research reactors and…

High Energy Physics - Phenomenology · Physics 2022-02-16 Jeffrey M. Berryman , Luis A. Delgadillo , Patrick Huber

In this paper, the possibility to exploit a high energy beta beam without massive detectors is discussed. The radioactive ions are boosted up to very high $\gamma$ with the neutrino beam pointing towards an instrumented surface located at a…

High Energy Physics - Phenomenology · Physics 2009-11-10 F. Terranova , A. Marotta , P. Migliozzi , M. Spinetti

The successful measurements of the smallest neutrino mixing angle, $\theta_{13}$, in 2012 by the short (1$\sim$2 km) baseline reactor neutrinos experiments, Daya Bay, RENO, and Double Chooz, have triggered a golden age of neutrino physics.…

High Energy Physics - Experiment · Physics 2017-02-01 Seon-Hee Seo

The EUROnu project has studied three possible options for future, high intensity neutrino oscillation facilities in Europe. The first is a Super Beam, in which the neutrinos come from the decay of pions created by bombarding targets with a…

Accelerator Physics · Physics 2013-05-20 T. R. Edgecock , O. Caretta , T. Davenne , C. Densham , M. Fitton , D. Kelliher , P. Loveridge , S. Machida , C. Prior , C. Rogers , M. Rooney , J. Thomason , D. Wilcox , E. Wildner , I. Efthymiopoulos , R. Garoby , S. Gilardoni , C. Hansen , E. Benedetto , E. Jensen , A. Kosmicki , M. Martini , J. Osborne , G. Prior , T. Stora , T. Melo-Mendonca , V. Vlachoudis , C. Waaijer , P. Cupial , A. Chancé , A. Longhin , J. Payet , M. Zito , E. Baussan , C. Bobeth , E. Bouquerel , M. Dracos , G. Gaudiot , B. Lepers , F. Osswald , P. Poussot , N. Vassilopoulos , J. Wurtz , V. Zeter , J. Bielski , M. Kozien , L. Lacny , B. Skoczen , B. Szybinski , A. Ustrycka , A. Wroblewski , M. Marie-Jeanne , P. Balint , C. Fourel , J. Giraud , J. Jacob , T. Lamy , L. Latrasse , P. Sortais , T. Thuillier , S. Mitrofanov , M. Loiselet , Th. Keutgen , Th. Delbar , F. Debray , C. Trophine , S. Veys , C. Daversin , V. Zorin , I. Izotov , V. Skalyga , G. Burt , A. C. Dexter , V. L. Kravchuk , T. Marchi , M. Cinausero , F. Gramegna , G. De Angelis , G. Prete , G. Collazuol , M. Laveder , M. Mazzocco , M. Mezzetto , C. Signorini , E. Vardaci , A. Di Nitto , A. Brondi , G. La Rana , P. Migliozzi , R. Moro , V. Palladino , N. Gelli , D. Berkovits , M. Hass , T. Y. Hirsh , M. Schaumann , A. Stahl , J. Wehner , A. Bross , J. Kopp , D. Neuffer , R. Wands , R. Bayes , A. Laing , P. Soler , S. K. Agarwalla , A. Cervera Villanueva , A. Donini , T. Ghosh , J. J. Gómez Cadenas , P. Hernández , J. Martín-Albo , O. Mena , J. Burguet-Castell , L. Agostino , M. Buizza-Avanzini , M. Marafini , T. Patzak , A. Tonazzo , D. Duchesneau , L. Mosca , M. Bogomilov , Y. Karadzhov , R. Matev , R. Tsenov , E. Akhmedov , M. Blennow , M. Lindner , T. Schwetz , E. Fernández Martinez , M. Maltoni , J. Menéndez , C. Giunti , M. C. González García , J. Salvado , P. Coloma , P. Huber , T. Li , J. López-Pavón , C. Orme , S. Pascoli , D. Meloni , J. Tang , W. Winter , T. Ohlsson , H. Zhang , L. Scotto-Lavina , F. Terranova , M. Bonesini , L. Tortora , A. Alekou , M. Aslaninejad , C. Bontoiu , A. Kurup , L. J. Jenner , K. Long , J. Pasternak , J. Pozimski , J. J. Back , P. Harrison , K. Beard , A. Bogacz , J. S. Berg , D. Stratakis , H. Witte , P. Snopok , N. Bliss , M. Cordwell , A. Moss , S. Pattalwar , M. Apollonio

Beta Beams are designed to produce pure (anti)electron neutrino beams and could be an elegant and powerful option for the search of leptonic CP violating processes. In this paper will be quantified the physics reach of a CERN based Beta…

High Energy Physics - Experiment · Physics 2008-11-26 Mauro Mezzetto

I discuss why and how powerful is the two-detector setting in neutrino oscillation experiments. I cover three concrete examples: (1) reactor \theta_{13} experiments, (2) T2KK, Tokai-to-Kamioka-Korea two-detector complex for measuring CP…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hisakazu Minakata

New generation experiments on search for neutrinoless double beta decay with sensitivity to effective Majorana neutrino mass on the level $\sim$ 3-5 meV is discussed. Possible restrictions at achievement of this purpose (possibility to…

Nuclear Experiment · Physics 2015-05-30 A. S. Barabash

We present an optimization procedure for neutrino beams which could be produced at CERN and aimed to a set of seven possible underground sites in Europe with distances ranging from 130 km to 2300 km. Studies on the feasibility of a next…

Instrumentation and Detectors · Physics 2012-06-20 A. Longhin

We propose a method to measure the neutrino mass kinematically using beams of ions which undergo beta decay. The idea is to tune the ion beam momentum so that in most decays, the electron is forward moving with respect to the beam, and only…

High Energy Physics - Phenomenology · Physics 2009-12-04 Mats Lindroos , Bob McElrath , Christopher Orme , Thomas Schwetz

The term beta-beam has been coined for the production of a pure beam of electron neutrinos or their antiparticles through the decay of radioactive ions circulating in a storage ring. This concept requires radioactive ions to be accelerated…

Accelerator Physics · Physics 2016-09-08 Mats Lindroos , the beta-beam Working Group

The precision and discovery potential of a neutrino factory based on muon storage rings is summarized. For three-family neutrino oscillations, we analyze how to measure or severely constraint the angle $\theta_{13}$, CP violation, MSW…

High Energy Physics - Phenomenology · Physics 2015-06-25 A. Cervera , A. Donini , M. B. Gavela , J. J. Gomez Cadenas , P. Hernandez , O. Mena , S. Rigolin

We perform a comprehensive study of the ability of the Deep Underground Neutrino Experiment (DUNE) to answer outstanding questions in the neutrino sector. We consider the sensitivities to the mass hierarchy, the octant of \theta_{23} and to…

High Energy Physics - Phenomenology · Physics 2016-03-04 Vernon Barger , Atri Bhattacharya , Animesh Chatterjee , Raj Gandhi , Danny Marfatia , Mehedi Masud

We examine the prospects of making a joint analysis of neutrino oscillation at two baselines with neutrino superbeams. Assuming narrow band superbeams and a 100 kt water Cerenkov calorimeter, we calculate the event rates and sensitivities…

High Energy Physics - Phenomenology · Physics 2008-11-26 Y. F. Wang , K. Whisnant , Z. Xiong , Jin Min Yang , Bing-Lin Young

The possibility of making a low cost, very intense high energy proton source at the Brookhaven Alternating Gradient Synchrotron (AGS) along with the forthcoming new large underground detectors at either the National Underground Science…

High Energy Physics - Experiment · Physics 2007-05-23 D. Beavis

Hyper-Kamiokande will be a next generation underground water Cherenkov detector with a total (fiducial) mass of 0.99 (0.56) million metric tons, approximately 20 (25) times larger than that of Super-Kamiokande. One of the main goals of…

Instrumentation and Detectors · Physics 2015-01-20 Kamiokande Working Group , K. Abe , H. Aihara , C. Andreopoulos , I. Anghel , A. Ariga , T. Ariga , R. Asfandiyarov , M. Askins , J. J. Back , P. Ballett , M. Barbi , G. J. Barker , G. Barr , F. Bay , P. Beltrame , V. Berardi , M. Bergevin , S. Berkman , T. Berry , S. Bhadra , F. d. M. Blaszczyk , A. Blondel , S. Bolognesi , S. B. Boyd , A. Bravar , C. Bronner , F. S. Cafagna , G. Carminati , S. L. Cartwright , M. G. Catanesi , K. Choi , J. H. Choi , G. Collazuol , G. Cowan , L. Cremonesi , G. Davies , G. De Rosa , C. Densham , J. Detwiler , D. Dewhurst , F. Di Lodovico , S. Di Luise , O. Drapier , S. Emery , A. Ereditato , P. Fernandez , T. Feusels , A. Finch , M. Fitton , M. Friend , Y. Fujii , Y. Fukuda , D. Fukuda , V. Galymov , K. Ganezer , M. Gonin , P. Gumplinger , D. R. Hadley , L. Haegel , A. Haesler , Y. Haga , B. Hartfiel , M. Hartz , Y. Hayato , M. Hierholzer , J. Hill , A. Himmel , S. Hirota , S. Horiuchi , K. Huang , A. K. Ichikawa , T. Iijima , M. Ikeda , J. Imber , K. Inoue , J. Insler , R. A. Intonti , T. Irvine , T. Ishida , H. Ishino , M. Ishitsuka , Y. Itow , A. Izmaylov , B. Jamieson , H. I. Jang , M. Jiang , K. K. Joo , C. K. Jung , A. Kaboth , T. Kajita , J. Kameda , Y. Karadhzov , T. Katori , E. Kearns , M. Khabibullin , A. Khotjantsev , J. Y. Kim , S. B. Kim , Y. Kishimoto , T. Kobayashi , M. Koga , A. Konaka , L. L. Kormos , A. Korzenev , Y. Koshio , W. R. Kropp , Y. Kudenko , T. Kutter , M. Kuze , L. Labarga , J. Lagoda , M. Laveder , M. Lawe , J. G. Learned , I. T. Lim , T. Lindner , A. Longhin , L. Ludovici , W. Ma , L. Magaletti , K. Mahn , M. Malek , C. Mariani , L. Marti , J. F. Martin , C. Martin , P. P. J. Martins , E. Mazzucato , N. McCauley , K. S. McFarland , C. McGrew , M. Mezzetto , H. Minakata , A. Minamino , S. Mine , O. Mineev , M. Miura , J. Monroe , T. Mori , S. Moriyama , T. Mueller , F. Muheim , M. Nakahata , K. Nakamura , T. Nakaya , S. Nakayama , M. Needham , T. Nicholls , M. Nirkko , Y. Nishimura , E. Noah , J. Nowak , H. Nunokawa , H. M. O'Keeffe , Y. Okajima , K. Okumura , S. M. Oser , E. O'Sullivan , R. A. Owen , Y. Oyama , J. Perez , M. Y. Pac , V. Palladino , J. L. Palomino , V. Paolone , D. Payne , O. Perevozchikov , J. D. Perkin , C. Pistillo , S. Playfer , M. Posiadala-Zezula , J. -M. Poutissou , B. Quilain , M. Quinto , E. Radicioni , P. N. Ratoff , M. Ravonel , M. Rayner , A. Redij , F. Retiere , C. Riccio , E. Richard , E. Rondio , H. J. Rose , M. Ross-Lonergan , C. Rott , S. D. Rountree , A. Rubbia , R. Sacco , M. Sakuda , M. C. Sanchez , E. Scantamburlo , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , A. Shaikhiev , I. Shimizu , M. Shiozawa , S. Short , G. Sinnis , M. B. Smy , J. Sobczyk , H. W. Sobel , T. Stewart , J. L. Stone , Y. Suda , Y. Suzuki , A. T. Suzuki , R. Svoboda , R. Tacik , A. Takeda , A. Taketa , Y. Takeuchi , H. A. Tanaka , H. K. M. Tanaka , H. Tanaka , R. Terri , L. F. Thompson , M. Thorpe , S. Tobayama , N. Tolich , T. Tomura , C. Touramanis , T. Tsukamoto , M. Tzanov , Y. Uchida , M. R. Vagins , G. Vasseur , R. B. Vogelaar , C. W. Walter , D. Wark , M. O. Wascko , A. Weber , R. Wendell , R. J. Wilkes , M. J. Wilking , J. R. Wilson , T. Xin , K. Yamamoto , C. Yanagisawa , T. Yano , S. Yen , N. Yershov , M. Yokoyama , M. Zito

The best method of measuring CP violating effect in neutrino oscillation experiments is to construct and use a neutrino beam made of an ideal mixture of $\bar{\nu}_e$ and $\nu_e$ of monochromatic lines. The conceptual design of such a beam…

High Energy Physics - Experiment · Physics 2011-05-25 A. Fukumi , I. Nakano , H. Nanjo , N. Sasao , S. Sato , M. Yoshimura

In this paper, we discuss the possibilities offered to neutrino physics by the upgrades of the CERN accelerator complex. Emphasis is on the physics reach of a medium $\gamma$ (350-580) $\beta$-beam that fully exploits the improvements in…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Donini , E. Fernandez , P. Migliozzi , S. Rigolin , L. Scotto Lavina , T. Tabarelli de Fatis , F. Terranova

In the context of neutrino factories, we review the solution of the degeneracies in the neutrino oscillation parameters. In particular, we have set limits to $\sin^2 2\theta_{13}$ in order to accomplish the unambiguous determination of…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. M. Gago , J. Jones-Perez

It is proposed to complement the ESS proton linac with equipment that would enable the production, concurrently with the production of the planned ESS beam used for neutron production, of a 5 MW beam of 10$^{23}$ 2.5 GeV protons per year in…

High Energy Physics - Experiment · Physics 2013-02-12 E. Baussan , M. Dracos , T. Ekelof , E. Fernandez Martinez , H. Ohman , N. Vassilopoulos