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In order to calibrate the Super-Kamiokande experiment for solar neutrino measurements, a linear accelerator (LINAC) for electrons was installed at the detector. LINAC data were taken at various positions in the detector volume, tracking the…

High Energy Physics - Experiment · Physics 2015-06-25 Kamiokande Collaboration

T2K is a neutrino oscillation experiment with a 295 km long baseline between the far detector, Super-Kamiokande, and a suite of near detectors to study $\nu_\mu/\bar{\nu}_\mu$ disappearance and $\nu_e/\bar{\nu}_e$ appearance in a…

High Energy Physics - Experiment · Physics 2024-05-13 T. Nosek

We summarize the status of Deep Underground Neutrino Experiment (DUNE) Offline Software and Computing program. We describe plans for the computing infrastructure needed to acquire, catalog, reconstruct, simulate and analyze the data from…

Accelerator Physics · Physics 2023-12-19 Michael Kirby

We investigate the precision with which the supernova neutrino spectra can be reconstructed in water Cherenkov detectors, in particular the large scale Hyper-Kamiokande and Super-Kamiokande. To this aim, we consider quasi-thermal neutrino…

High Energy Physics - Phenomenology · Physics 2018-04-25 Andrea Gallo Rosso , Francesco Vissani , Maria Cristina Volpe

T2K is a long-baseline neutrino oscillation experiment, in which a muon neutrino beam is produced at J-PARC and detected 295 km away at the Super-Kamiokande detector. The T2K experiment observed electron-neutrino appearance in 2012. This…

High Energy Physics - Experiment · Physics 2015-08-26 M. Ravonel Salzgeber

The Super-Kamiokande best global fit, which includes data from SNO, Gallium and Chlorine experiments, results in a hep neutrino contribution to the signals that, even after oscillation, is greater than the SSM prediction. The solar hep…

High Energy Physics - Phenomenology · Physics 2014-11-17 Massimo Coraddu , Marcello Lissia , Giuseppe Mezzorani , Piero Quarati

Studying the atmospheric neutrino oscillation probabilities below 2 GeV with a multi-megaton Cherenkov detector allows for a measurement of the leptonic CP-phase $\delta_{CP}$. The most relevant CP-sensitive energy range is below the…

High Energy Physics - Experiment · Physics 2019-07-31 Jannik Hofestädt , Marc Bruchner , Thomas Eberl

We study physics potential of placing a far detector in the east coast of Korea, where the off-axis beam from J-PARC at Tokai village for the T2K project has significant intensity at a few GeV range. In particular we examine the capability…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kaoru Hagiwara , Naotoshi Okamura , Ken-ichi Senda

Baryon number violation appears in many contexts. It is a requirement for baryogenesis and is a consequence of Grand Unified Theories (GUTs), which predict nucleon decay. Nucleon decay searches provide the most direct way to test baryon…

High Energy Physics - Experiment · Physics 2019-08-14 Volodymyr Takhistov

The three neutrino model has 9 physical parameters, 3 neutrino masses, 3 mixing angles and 3 CP violating phases. Among them, neutrino oscillation experiments can probe 6 parameters: 2 mass squared differences, 3 mixing angles, and 1 CP…

High Energy Physics - Phenomenology · Physics 2009-11-10 Kaoru Hagiwara

It is said that the finding of the maximum oscillation in neutrino oscillation by Super-Kamiokande is one of the major achievements of the SK. In present paper, we examine the assumption made by Super-Kamiokande Collaboration that the…

High Energy Physics - Experiment · Physics 2010-07-23 E. Konishi , Y. Minorikawa , V. I. Galkin , M. Ishiwata , I. Nakamura , N. Takahashi , M. Kato , A. Misaki

We report the largest scale deep learning with High Performance Computing (HPC) to physics analysis with the CMS simulation data in proton-proton collisions at 13 TeV. We build a Convolutional Neural Network (CNN) model that takes low-level…

We develop a new discrimination procedure for separating electron neutrinos from muon neutrinos, based on detailed simulations carried out with GEANT3.21 and with mean angular distribution functions and their relative fluctuations. Using…

High Energy Physics - Experiment · Physics 2008-08-07 V. I. Galkin , A. M. Anokhina , E. Konishi , A. Misaki

CUPID is a proposed future tonne-scale bolometric neutrinoless double beta decay ($0\nu\beta\beta$) experiment to probe the Majorana nature of neutrinos and discover Lepton Number Violation in the so-called inverted hierarchy region of the…

Instrumentation and Detectors · Physics 2019-07-23 The CUPID Interest Group

In this paper we place new bounds on CPT violation in the solar neutrino sector analyzing the results from solar experiments and KamLAND. We also discuss the sensitivity of the next-generation experiments DUNE and Hyper-Kamiokande, which…

High Energy Physics - Phenomenology · Physics 2023-05-12 Gabriela Barenboim , Pablo Martínez-Miravé , Christoph A. Ternes , Mariam Tórtola

Large liquid scintillation detectors have been generally dedicated to low energy neutrino measurements, in the MeV energy region (as for example, KamLAND and Borexino). Herein we describe the potential employment of large detectors (>1…

High Energy Physics - Experiment · Physics 2009-02-25 John G. Learned

Exponential increases in scientific experimental data are outstripping the rate of progress in silicon technology. As a result, heterogeneous combinations of architectures and process or device technologies are increasingly important to…

Distributed, Parallel, and Cluster Computing · Computer Science 2024-07-02 Wilkie Olin-Ammentorp , Xingfu Wu , Andrew A. Chien

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

T2K is a long-baseline neutrino oscillation experiment, in which a muon-neutrino beam is directed over a 295 km baseline from the J-PARC facility to the Super-Kamiokande detector. This allows neutrino oscillation to be studied in two…

High Energy Physics - Experiment · Physics 2019-08-14 Kirsty Duffy

We present a combined analysis of fully-contained, partially-contained and upward-going muon atmospheric neutrino data from a 1489 day exposure of the Super--Kamiokande detector. The data samples span roughly five decades in neutrino…

High Energy Physics - Experiment · Physics 2008-11-26 Kamiokande Collaboration