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We evaluate the probability of future neutrino oscillation facilities to discover leptonic CP violation and/or measure the neutrino mass hierarchy. We study how this probability is affected by positive or negative hints for these…

High Energy Physics - Phenomenology · Physics 2015-06-15 Mattias Blennow , Pilar Coloma , Andrea Donini , Enrique Fernandez-Martinez

NOvA experiment has reoptimized its event selection criteria in light of the recently measured moderately large value of theta(13). We study the improvement in the sensitivity to the neutrino mass hierarchy and to leptonic CP violation due…

High Energy Physics - Phenomenology · Physics 2013-03-05 Sanjib Kumar Agarwalla , Suprabh Prakash , Sushant K. Raut , S. Uma Sankar

The Daya Bay and RENO experiments have recently observed a non-zero $\theta_{13}$ at more than $5\sigma$ CL. This has important consequences for future neutrino oscillation experiments. We analyze these within the LAGUNA design study which…

High Energy Physics - Phenomenology · Physics 2012-06-19 Pilar Coloma , Tracey Li , Silvia Pascoli

Precision measurement of the neutrino mixing parameters and the determination of mass hierarchy are the primary goals of the present and upcoming neutrino experiments. In this work, we study the sensitivity of T2K,NO$\nu$A and LBNE…

High Energy Physics - Phenomenology · Physics 2015-06-22 K. N. Deepthi , C. Soumya , R. Mohanta

Recent data from long-baseline neutrino oscillation experiments have provided new information on \theta_{13}, hinting that 0.01\lesssim sin^2 2\theta_{13} \lesssim 0.1 at 2 sigma C.L. Confirmation of this result with high significance will…

High Energy Physics - Phenomenology · Physics 2015-05-30 Sanjib Kumar Agarwalla , Tracey Li , Andre Rubbia

We compare the physics potential of the upcoming neutrino oscillation experiments Daya Bay, Double Chooz, NOvA, RENO, and T2K based on their anticipated nominal luminosities and schedules. After discussing the sensitivity to theta_{13} and…

High Energy Physics - Phenomenology · Physics 2009-11-18 Patrick Huber , Manfred Lindner , Thomas Schwetz , Walter Winter

A high-power neutrino superbeam experiment at the ESS facility has been proposed such that the source-detector distance falls at the second oscillation maximum, giving very good sensitivity towards establishing CP violation. In this work,…

High Energy Physics - Phenomenology · Physics 2015-06-19 Sanjib Kumar Agarwalla , Sandhya Choubey , Suprabh Prakash

We discuss the neutrino mass hierarchy determination with atmospheric neutrinos in PINGU (Precision IceCube Next Generation Upgrade), based on a simulation with the GLoBES software including the full three flavor framework and parameter…

High Energy Physics - Phenomenology · Physics 2013-08-09 Walter Winter

We perform a comparison of the different future neutrino oscillation experiments based on the achievable precision in the determination of the fundamental parameters theta_{13} and the CP phase, delta, assuming that theta_{13} is in the…

High Energy Physics - Phenomenology · Physics 2015-06-04 Pilar Coloma , Andrea Donini , Enrique Fernandez-Martinez , Pilar Hernandez

The two long-baseline experiments T2K and NO$\nu$A have recently presented new findings. T2K has shown the first $\bar \nu_e$ appearance data while NO$\nu$A has released the first $\nu_e$ appearance results. These data are of particular…

High Energy Physics - Phenomenology · Physics 2016-05-04 Antonio Palazzo

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

Leptonic \textit{CP} violation search, neutrino mass hierarchy determination, and the precision measurement of oscillation parameters for a unitary test of the leptonic mixing matrix are among the major targets of the ongoing and future…

High Energy Physics - Phenomenology · Physics 2021-07-07 S. Cao , A. Nath , T. V. Ngoc , P. T. Quyen , N. T. Hong Van , Ng. K. Francis

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 discovery of neutrino mixing and oscillations over the past decade provides firm evidence for new physics beyond the Standard Model. Recently, theta13 has been determined to be moderately large, quite close to its previous upper bound.…

High Energy Physics - Phenomenology · Physics 2014-01-21 Sanjib Kumar Agarwalla

One of the unknown parameters in neutrino oscillations is the octant of the mixing angle theta_{23}. In this paper, we discuss the possibility of determining the octant of theta_{23} in the long baseline experiments T2K and NOvA in…

High Energy Physics - Phenomenology · Physics 2013-07-11 Animesh Chatterjee , Pomita Ghoshal , Srubabati Goswami , Sushant K. Raut

One of the main goals of the Long Baseline Neutrino Oscillation experiment (LBNO) experiment is to study the L/E behaviour of the electron neutrino appearance probability in order to determine the unknown phase $\delta_{CP}$. In the…

Instrumentation and Detectors · Physics 2014-11-11 M. Calviani , S. Di Luise , V. Galymov , P. Velten

Among three leptonic mixing angles, $\theta_{23}$ angle, which characterizes the fractional contribution of two flavor eigenstates $\nu_{\mu}$ and $\nu_{\tau}$ to the third mass eigenstate $\nu_3$, is known to be the largest but the least…

High Energy Physics - Phenomenology · Physics 2024-10-29 Son Cao , P. T. Quyen , N. T. Hong Van , Ankur Nath , T. V. Ngoc

Very soon a new generation of reactor and accelerator neutrino oscillation experiments - Double Chooz, Daya Bay, Reno and T2K - will seek for oscillation signals generated by the mixing parameter theta_13. The knowledge of this angle is a…

High Energy Physics - Experiment · Physics 2014-11-20 R. Battiston , M. Mezzetto , P. Migliozzi , F. Terranova

We study the physics potential of future long-baseline neutrino oscillation experiments at large $\theta_{13}$, focusing especially on systematic uncertainties. We discuss superbeams, \bbeams, and neutrino factories, and for the first time…

High Energy Physics - Phenomenology · Physics 2013-03-14 Pilar Coloma , Patrick Huber , Joachim Kopp , Walter Winter

In order to address some fundamental questions in neutrino physics a wide, future programme of neutrino oscillation experiments is currently under discussion. Among those, long baseline experiments will play a crucial role in providing…

High Energy Physics - Phenomenology · Physics 2009-03-19 Davide Meloni , Olga Mena , Christopher Orme , Sergio Palomares-Ruiz , Silvia Pascoli
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