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Related papers: Neutrino oscillations at dual baselines

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We discuss the prospects of exploring the neutrino mass parameters with a CERN based Beta-beam experiment using two different detectors at two different baselines. The proposed set-up consists of a 50 kton iron calorimeter (ICAL) at a…

High Energy Physics - Phenomenology · Physics 2009-04-14 Sanjib Kumar Agarwalla , Sandhya Choubey , Amitava Raychaudhuri

In this paper, we discuss a possibility of studying properties of dark energy in long baseline neutrino oscillation experiments. We consider two types of models of neutrino dark energy. For one type of models the scalar field is taken to be…

High Energy Physics - Phenomenology · Physics 2011-08-31 Pei-Hong Gu , Xiao-Jun Bi , Bo Feng , Bing-Lin Young , Xinmin Zhang

Neutrino mixing parameters are subject to quantum corrections and hence are scale dependent. This means that the mixing parameters associated to the production and detection of neutrinos need not coincide since these processes are…

High Energy Physics - Phenomenology · Physics 2022-06-14 K. S. Babu , Vedran Brdar , André de Gouvêa , Pedro A. N. Machado

The next generation neutrino observatory proposed by the LBNO collaboration will address fundamental questions in particle and astroparticle physics. The experiment consists of a far detector, in its first stage a 20 kt LAr double phase TPC…

High Energy Physics - Phenomenology · Physics 2014-01-21 LBNO Collaboration , S. K. Agarwalla , L. Agostino , M. Aittola , A. Alekou , B. Andrieu , D. Angus , F. Antoniou , A. Ariga , T. Ariga , R. Asfandiyarov , D. Autiero , P. Ballett , I. Bandac , D. Banerjee , G. J. Barker , G. Barr , W. Bartmann , F. Bay , V. Berardi , I. Bertram , O. Bésida , A. M. Blebea-Apostu , A. Blondel , M. Bogomilov , E. Borriello , S. Boyd , I. Brancus , A. Bravar , M. Buizza-Avanzini , F. Cafagna , M. Calin , M. Calviani , M. Campanelli , C. Cantini , O. Caretta , G. Cata-Danil , M. G. Catanesi , A. Cervera , S. Chakraborty , L. Chaussard , D. Chesneanu , F. Chipesiu , G. Christodoulou , J. Coleman , P. Crivelli , T. Davenne , J. Dawson , I. De Bonis , J. De Jong , Y. Déclais , P. Del Amo Sanchez , A. Delbart , C. Densham , F. Di Lodovico , S. Di Luise , D. Duchesneau , J. Dumarchez , I. Efthymiopoulos , A. Eliseev , S. Emery , K. Enqvist , T. Enqvist , L. Epprecht , A. Ereditato , A. N. Erykalov , T. Esanu , A. J. Finch , M. D. Fitton , D. Franco , V. Galymov , G. Gavrilov , A. Gendotti , C. Giganti , B. Goddard , J. J. Gomez , C. M. Gomoiu , Y. A. Gornushkin , P. Gorodetzky , N. Grant , A. Haesler , M. D. Haigh , T. Hasegawa , S. Haug , M. Hierholzer , J. Hissa , S. Horikawa , K. Huitu , J. Ilic , A. N. Ioannisian , A. Izmaylov , A. Jipa , K. Kainulainen , T. Kalliokoski , Y. Karadzhov , J. Kawada , M. Khabibullin , A. Khotjantsev , E. Kokko , A. N. Kopylov , L. L. Kormos , A. Korzenev , S. Kosyanenko , I. Kreslo , D. Kryn , Y. Kudenko , V. A. Kudryavtsev , J. Kumpulainen , P. Kuusiniemi , J. Lagoda , I. Lazanu , J. -M. Levy , R. P. Litchfield , K. Loo , P. Loveridge , J. Maalampi , L. Magaletti , R. M. Margineanu , J. Marteau , C. Martin-Mari , V. Matveev , K. Mavrokoridis , E. Mazzucato , N. McCauley , A. Mercadante , O. Mineev , A. Mirizzi , B. Mitrica , B. Morgan , M. Murdoch , S. Murphy , K. Mursula , S. Narita , D. A. Nesterenko , K. Nguyen , K. Nikolics , E. Noah , Yu. Novikov , H. O'Keeffe , J. Odell , A. Oprima , V. Palladino , Y. Papaphilippou , S. Pascoli , T. Patzak , D. Payne , M. Pectu , E. Pennacchio , L. Periale , H. Pessard , C. Pistillo , B. Popov , P. Przewlocki , M. Quinto , E. Radicioni , Y. Ramachers , P. N. Ratoff , M. Ravonel , M. Rayner , F. Resnati , O. Ristea , A. Robert , E. Rondio , A. Rubbia , K. Rummukainen , R. Sacco , A. Saftoiu , K. Sakashita , J. Sarkamo , F. Sato , N. Saviano , E. Scantamburlo , F. Sergiampietri , D. Sgalaberna , E. Shaposhnikova , M. Slupecki , M. Sorel , N. J. C. Spooner , A. Stahl , D. Stanca , R. Steerenberg , A. R. Sterian , P. Sterian , B. Still , S. Stoica , T. Strauss , J. Suhonen , V. Suvorov , M. Szeptycka , R. Terri , L. F. Thompson , G. Toma , A. Tonazzo , C. Touramanis , W. H. Trzaska , R. Tsenov , K. Tuominen , A. Vacheret , M. Valram , G. Vankova-Kirilova , F. Vanucci , G. Vasseur , F. Velotti , P. Velten , T. Viant , H. Vincke , A. Virtanen , A. Vorobyev , D. Wark , A. Weber , M. Weber , C. Wiebusch , J. R. Wilson , S. Wu , N. Yershov , J. Zalipska , M. Zito

We propose a new method for measuring CP violation in neutrino oscillation experiments. The idea is to isolate the term due to the CP-violating phase out of the oscillation probability by taking difference between yields of two (or three)…

High Energy Physics - Phenomenology · Physics 2011-02-24 Hisakazu Minakata , Hiroshi Nunokawa

The Tokai to Kamioka (T2K) experiment uses a beam of muon neutrinos, produced at the J-PARC facility on the east coast of Japan, to study neutrino oscillations driven by the $\Delta m_{\textrm{atm}}^{2}$ mass splitting. A suite of near…

High Energy Physics - Experiment · Physics 2015-01-20 Martin David Haigh

There are three parameter degeneracies inherent in the three--neutrino analysis of long--baseline neutrino experiments. We develop a systematic method for determining whether or not a set of measurements in neutrino oscillation appearance…

High Energy Physics - Phenomenology · Physics 2008-11-26 V. Barger , D. Marfatia , K. Whisnant

The proposed Long Baseline Neutrino Observatory (LBNO) initially consists of $\sim 20$ kton liquid double phase TPC complemented by a magnetised iron calorimeter, to be installed at the Pyh\"asalmi mine, at a distance of 2300 km from CERN.…

High Energy Physics - Phenomenology · Physics 2014-12-03 LBNO Collaboration , S. K. Agarwalla , L. Agostino , M. Aittola , A. Alekou , B. Andrieu , F. Antoniou , R. Asfandiyarov , D. Autiero , O. Bésida , A. Balik , P. Ballett , I. Bandac , D. Banerjee , W. Bartmann , F. Bay , B. Biskup , A. M. Blebea-Apostu , A. Blondel , M. Bogomilov , S. Bolognesi , E. Borriello , I. Brancus , A. Bravar , M. Buizza-Avanzini , D. Caiulo , M. Calin , M. Calviani , M. Campanelli , C. Cantini , G. Cata-Danil , S. Chakraborty , N. Charitonidis , L. Chaussard , D. Chesneanu , F. Chipesiu , P. Crivelli , J. Dawson , I. De Bonis , Y. Declais , P. Del Amo Sanchez , A. Delbart , S. Di Luise , D. Duchesneau , J. Dumarchez , I. Efthymiopoulos , A. Eliseev , S. Emery , T. Enqvist , K. Enqvist , L. Epprecht , A. N. Erykalov , T. Esanu , D. Franco , M. Friend , V. Galymov , G. Gavrilov , A. Gendotti , C. Giganti , S. Gilardoni , B. Goddard , C. M. Gomoiu , Y. A. Gornushkin , P. Gorodetzky , A. Haesler , T. Hasegawa , S. Horikawa , K. Huitu , A. Izmaylov , A. Jipa , K. Kainulainen , Y. Karadzhov , M. Khabibullin , A. Khotjantsev , A. N. Kopylov , A. Korzenev , S. Kosyanenko , D. Kryn , Y. Kudenko , P. Kuusiniemi , I. Lazanu , C. Lazaridis , J. -M. Levy , K. Loo , J. Maalampi , R. M. Margineanu , J. Marteau , C. Martin-Mari , V. Matveev , E. Mazzucato , A. Mefodiev , O. Mineev , A. Mirizzi , B. Mitrica , S. Murphy , T. Nakadaira , S. Narita , D. A. Nesterenko , K. Nguyen , K. Nikolics , E. Noah , Yu. Novikov , A. Oprima , J. Osborne , T. Ovsyannikova , Y. Papaphilippou , S. Pascoli , T. Patzak , M. Pectu , E. Pennacchio , L. Periale , H. Pessard , B. Popov , M. Ravonel , M. Rayner , F. Resnati , O. Ristea , A. Robert , A. Rubbia , K. Rummukainen , A. Saftoiu , K. Sakashita , F. Sanchez-Galan , J. Sarkamo , N. Saviano , E. Scantamburlo , F. Sergiampietri , D. Sgalaberna , E. Shaposhnikova , M. Slupecki , D. Smargianaki , D. Stanca , R. Steerenberg , A. R. Sterian , P. Sterian , S. Stoica , C. Strabel , J. Suhonen , V. Suvorov , G. Toma , A. Tonazzo , W. H. Trzaska , R. Tsenov , K. Tuominen , M. Valram , G. Vankova-Kirilova , F. Vannucci , G. Vasseur , F. Velotti , P. Velten , V. Venturi , T. Viant , S. Vihonen , H. Vincke , A. Vorobyev , A. Weber , S. Wu , N. Yershov , L. Zambelli , M. Zito

We study the method to test the unitarity of the lepton mixing matrix by using only the long baseline neutrino oscillation experiments, such as the combination of the T2HK experiment and the one with the $\nu_e$ beam from a future neutrino…

High Energy Physics - Phenomenology · Physics 2026-03-31 Ryuichiro Kitano , Joe Sato , Sho Sugama

Rector neutrinos have been a tool to investigate neutrino properties for more than 60 years. The reactor neutrino flux was measured throughout 80s-90s. In the 2000s, reactor neutrino oscillations at large baselines were observed by the…

High Energy Physics - Experiment · Physics 2018-12-11 Bedrich Roskovec

Many experiments are currently looking for evidence of neutrino mass in the form of neutrino oscillations. Oscillation probabilities are non-linear functions of the neutrino mixing matrix elements, so most comparisons of data to theory are…

High Energy Physics - Phenomenology · Physics 2007-05-23 Doris Jeanne Wagner

The determination of the ordering of the neutrino masses (the hierarchy) is probably a crucial prerequisite to understand the origin of lepton masses and mixings and to establish their relationship to the analogous properties in the quark…

High Energy Physics - Phenomenology · Physics 2008-11-26 Olga Mena , Hiroshi Nunokawa , Stephen Parke

We perform a calculation in quantum field theory of neutrino oscillation probabilities, where we include simultaneously the source, detector, and neutrino fields in the Hamiltonian. Within the appropriate limits associated with current…

High Energy Physics - Phenomenology · Physics 2018-07-18 Andrew Kobach , Aneesh V. Manohar , John McGreevy

T2K is a long-baseline neutrino oscillation experiment taking data since 2010. A neutrino beam is produced at the J-PARC accelerator in Japan and is sampled at a Near Detector complex 280 m from the neutrino production point and at the far…

High Energy Physics - Experiment · Physics 2022-09-21 L. Haegel

Recent $\nu_e$ appearance data from the Mini Booster Neutrino Experiment (MiniBooNE) are in support of the excess of events reported by the Liquid Scintillator Neutrino Detector (LSND), which provides an indirect hint for the existence of…

High Energy Physics - Phenomenology · Physics 2020-07-23 Rudra Majhi , Soumya C , Rukmani Mohanta

Next-generation long-baseline electron neutrino appearance experiments will seek to discover CP violation, determine the mass hierarchy and resolve the $\theta_{23}$ octant. In light of the recent precision measurements of $\theta_{13}$, we…

High Energy Physics - Experiment · Physics 2015-03-25 M. Bass , M. Bishai , D. Cherdack , M. Diwan , Z. Djurcic , J. Hernandez , B. Lundberg , V. Paolone , X. Qian , R. Rameika , L. Whitehead , R. J. Wilson , E. Worcester , G. Zeller

In order to make precision measurements of neutrino oscillations using few-GeV neutrino beams a detailed understanding of nuclear effects in neutrino scattering is essential. Recent studies have revealed that single-transverse kinematic…

High Energy Physics - Experiment · Physics 2019-08-14 Stephen Dolan , Xianguo Lu , Luke Pickering , Tomislav Vladisavljevic , Alfons Weber

The planned LBL experiments will be able to prove the hypothesis of flavor oscillation between muon and tau neutrinos. We explore the possibility of a second generation long baseline experiment at very long baseline, i.e. L in the range…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Campanelli , A. Bueno , A. Rubbia

We study the neutrino oscillation physics performance of the Long-Baseline Neutrino Experiment (LBNE) in various configurations. In particular, we compare the case of a surface detector at the far site augmented by a near detector, to that…

High Energy Physics - Phenomenology · Physics 2014-01-22 Vernon Barger , Atri Bhattacharya , Animesh Chatterjee , Raj Gandhi , Danny Marfatia , Mehedi Masud

We discuss to what extent future precision measurements of neutrino mixing observables will influence the information we can draw from a measurement of (or an improved limit on) neutrinoless double beta decay. Whereas the Delta m^2…

High Energy Physics - Phenomenology · Physics 2009-11-11 S. Choubey , W. Rodejohann
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