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The Universe is awash with tens-of-MeV neutrinos of all species coming from all past core-collapse supernovae. These have never been observed, but this state of affairs will change in the near future. In the less than ten years, the…

High Energy Physics - Phenomenology · Physics 2021-01-04 André de Gouvêa , Ivan Martinez-Soler , Yuber F. Perez-Gonzalez , Manibrata Sen

The T2K experiment is a long-baseline accelerator neutrino experiment using a near detector complex ND280 and a far detector, Super-Kamiokande. Neutrino interactions are detected by Cherenkov light in Super-Kamiokande in order to measure…

High Energy Physics - Experiment · Physics 2019-08-14 L. Haegel

The detection of astrophysical neutrinos by IceCube and the potential to constrain source models of ultra-high energy cosmic rays provide the motivation to develop instruments for the observation of neutrinos above $10^7$ GeV. Among the…

Instrumentation and Methods for Astrophysics · Physics 2019-07-23 A. Nepomuk Otte , Eliza Gazda , Eleanor Judd , John F. Krizmanic , Evgeny Kutzenzov , Oscar Romero Matamala , Patrick J. Reardon , Lawrence Wiencke

The KEK to Kamioka long-baseline neutrino experiment (K2K) is the first accelerator-based experiment with hundreds of km neutrino path length. K2K focuses on the study of the existence of neutrino oscillations in $\nu_{\mu}$ disappearance…

High Energy Physics - Experiment · Physics 2007-05-23 A. K. Ichikawa

We show that for recently discovered large values of theta(13), a superbeam with an average neutrino energy of ~ 5 GeV, such as those being proposed at CERN, if pointing to Super-Kamiokande (L = 8770 km), could reveal the neutrino mass…

High Energy Physics - Phenomenology · Physics 2015-06-04 Sanjib Kumar Agarwalla , Pilar Hernandez

In this paper, we investigate the impact in future megaton-scale water Cherenkov detectors of identifying proton Cherenkov rings. We estimate the expected event rates for detected neutral current and charged current quasi-elastic neutrino…

High Energy Physics - Phenomenology · Physics 2009-11-18 M. Fechner , C. W. Walter

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

We present the status of the development of a Cherenkov telescope to be flown on a long-duration balloon flight, the Extreme Universe Space Observatory Super Pressure Balloon 2 (EUSO-SPB2). EUSO-SPB2 is an approved NASA balloon mission that…

MEMPHYS (MEgaton Mass PHYSics) is a proposed large-scale water-Cherenkov experiment to be performed deep underground. It is dedicated to nucleon decay searches and the detection of neutrinos from supernovae, solar, and atmospheric…

Instrumentation and Detectors · Physics 2015-06-16 L. Agostino , M. Buizza-Avanzini , M. Marafini , T. Patzak , A. Tonazzo , M. Dracos , N. Vassilopoulos , D. Duchesneau , M. Mezzetto , L. Mosca

The T2K (Tokai to Kamioka) experiment is a second generation long baseline neutrino oscillation experiment located in Japan. The main goal is to probe the $\theta_{13}$ neutrino mixing parameter by looking for $\nu_{\mu}\to\nu_e$…

High Energy Physics - Experiment · Physics 2019-08-14 Alexander Izmaylov

We present a new strategy for measuring the electron neutrino mass ($\mnue$) by future detection of a Galactic supernova in large underground detectors such as the Super-Kamiokande (SK). This method is nearly model-independent and one can…

Astrophysics · Physics 2009-10-30 Tomonori Totani

The largest underground neutrino observatory, Super-Kamiokande, located near Kamioka, Japan has been collecting data since April 1996. It is located at a depth of roughly 2.7 kmwe in a zinc mine under a mountain, and has an effective area…

Astrophysics · Physics 2016-08-30 Kamiokande Collaboration , presented by J. G. Learned

The Tokai Intermediate Tank with Unoscillated Spectrum (TITUS) detector is a proposed addition to the Hyper-Kamiokande (HK) experiment located approximately 2 km from the J-PARC neutrino beam. The design consists of a 2 kton Gadolinium (Gd)…

Instrumentation and Detectors · Physics 2015-05-13 Pierre Lasorak , Nick Prouse

We present measurements of total neutron production from atmospheric neutrino interactions in water, analyzed as a function of electron-equivalent visible energy over a range of 30 MeV to 10 GeV. These results are based on 4,270 days of…

High Energy Physics - Experiment · Physics 2025-06-23 Kamiokande collaboration , S. Han , K. Abe , S. Abe , Y. Asaoka , C. Bronner , M. Harada , Y. Hayato , K. Hiraide , K. Hosokawa , K. Ieki , M. Ikeda , J. Kameda , Y. Kanemura , R. Kaneshima , Y. Kashiwagi , Y. Kataoka , S. Miki , S. Mine , M. Miura , S. Moriyama , M. Nakahata , S. Nakayama , Y. Noguchi , G. Pronost , K. Sato , K. Okamoto , H. Sekiya , H. Shiba , K. Shimizu , R. Shinoda , M. Shiozawa , Y. Sonoda , Y. Suzuki , A. Takeda , Y. Takemoto , A. Takenaka , H. Tanaka , T. Yano , T. Kajita , K. Okumura , R. Nishijima , T. Tashiro , T. Tomiya , X. Wang , S. Yoshida , P. Fernandez , L. Labarga , N. Ospina , D. Samudio , B. Zaldivar , B. W. Pointon , C. Yanagisawa , E. Kearns , J. L. Raaf , L. Wan , T. Wester , J. Bian , B. Cortez , N. J. Griskevich , M. B. Smy , H. W. Sobel , V. Takhistov , A. Yankelevich , J. Hill , M. C. Jang , S. H. Lee , D. H. Moon , R. G. Park , B. S. Yang , B. Bodur , K. Scholberg , C. W. Walter , A. Beauchêne , O. Drapier , A. Giampaolo , A. Ershova , Th. A. Mueller , A. D. Santos , P. Paganini , C. Quach , R. Rogly , T. Nakamura , J. S. Jang , L. N. Machado , F. P. Soler , J. G. Learned , K. Choi , N. Iovine , S. Cao , L. H. V. Anthony , D. Martin , N. W. Prouse , M. Scott , Y. Uchida , A. A. Sztuc , V. Berardi , N. F. Calabria , M. G. Catanesi , E. Radicioni , A. Langella , G. De Rosa , G. Collazuol , M. Feltre , F. Iacob , M. Mattiazzi , L. Ludovici , M. Gonin , L. Périssé , 23 B. Quilain , C. Fujisawa , S. Horiuchi , A. Kawabata , M. Kobayashi , Y. M. Liu , Y. Maekawa , Y. Nishimura , R. Okazaki , R. Akutsu , M. Friend , T. Hasegawa , T. Ishida , T. Kobayashi , M. Jakkapu , T. Matsubara , T. Nakadaira , K. Nakamura , Y. Oyama , A. Portocarrero Yrey , K. Sakashita , T. Sekiguchi , T. Tsukamoto , N. Bhuiyan , G. T. Burton , F. Di Lodovico , J. Gao , A. Goldsack , T. Katori , J. Migenda , R. M. Ramsden , Z. Xie , S. Zsoldos , T. Sone , A. T. Suzuki , Y. Takagi , Y. Takeuchi , S. Wada , H. Zhong , J. Feng , L. Feng , J. Hikida , J. R. Hu , Z. Hu , M. Kawaue , T. Kikawa , M. Mori , T. Nakaya , T. V. Ngoc , R. A. Wendell , K. Yasutome , S. J. Jenkins , N. McCauley , A. Tarrant , P. Mehta , M. Fanì , M. J. Wilking , Y. Fukuda , Y. Itow , H. Menjo , Y. Yoshioka , K. Ninomiya , J. Lagoda , S. M. Lakshmi , M. Mandal , P. Mijakowski , Y. S. Prabhu , J. Zalipska , M. Jia , J. Jiang , C. K. Jung , W. Shi , K. Hamaguchi , Y. Hino , H. Ishino , Y. Koshio , F. Nakanishi , S. Sakai , T. Tada , T. Tano , T. Ishizuka , G. Barr , D. Barrow , L. Cook , S. Samani , D. Wark , A. Holin , F. Nova , S. Jung , J. Y. Yang , J. Yoo , J. E. P. Fannon , L. Kneale , M. Malek , J. M. McElwee , T. Peacock , P. Stowell , M. D. Thiesse , L. F. Thompson , S. T. Wilson , H. Okazawa , S. M. Lakshmi , S. B. Kim , E. Kwon , M. W. Lee , J. W. Seo , I. Yu , A. K. Ichikawa , K. D. Nakamura , S. Tairafune , K. Nishijima , A. Eguchi , S. Goto , S. Kodama , Y. Mizuno , T. Muro , K. Nakagiri , Y. Nakajima , S. Shima , N. Taniuchi , E. Watanabe , M. Yokoyama , P. de Perio , S. Fujita , C. Jesús-Valls , K. Martens , Ll. Marti , K. M. Tsui , M. R. Vagins , J. Xia , M. Kuze , S. Izumiyama , R. Matsumoto , K. Terada , R. Asaka , M. Ishitsuka , H. Ito , Y. Ommura , N. Shigeta , M. Shinoki , M. Sugo , M. Wako , K. Yamauchi , T. Yoshida , Y. Nakano , F. Cormier , R. Gaur , V. Gousy-Leblanc , M. Hartz , A. Konaka , X. Li , B. R. Smithers , S. Chen , Y. Wu , B. D. Xu , A. Q. Zhang , B. Zhang , M. Girgus , P. Govindaraj , M. Posiadala-Zezula , S. B. Boyd , R. Edwards , D. Hadley , M. Nicholson , M. O'Flaherty , B. Richards , A. Ali , B. Jamieson , S. Amanai , D. Hamaguchi , A. Minamino , Y. Sasaki , R. Shibayama , R. Shimamura , S. Suzuki

The demand for underground labs for neutrino and rare event search experiments has been increasing over the last few decades. Yemilab, constructed in October 2022, is the first deep ($\sim$1~km) underground lab dedicated to science in…

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

The $\nu_\mu$ and $\nu_\tau$ neutrinos (and their antiparticles) from a Galactic core-collapse supernova can be observed in a water-\v{C}erenkov detector by the neutral-current excitation of $^{16}$O. The number of events expected is…

High Energy Physics - Phenomenology · Physics 2010-11-30 J. F. Beacom , P. Vogel

Cosmic-ray muons and especially their secondaries break apart nuclei ("spallation") and produce fast neutrons and beta-decay isotopes, which are backgrounds for low-energy experiments. In Super-Kamiokande, these beta decays are the dominant…

Instrumentation and Detectors · Physics 2015-12-02 Shirley Weishi Li , John F. Beacom

Modification of large water Cherenkov detectors by addition of gadolinium has been proposed. The large cross section for neutron capture on Gd will greatly improve the sensitivity to antielectron neutrinos from supernovae and reactors. A…

Instrumentation and Methods for Astrophysics · Physics 2019-08-14 Atsuko Kibayashi

Detecting supernova $\nu_e$ is essential for testing supernova and neutrino physics, but the yields are small and the backgrounds from other channels large, e.g., $\sim 10^2$ and $\sim 10^4$ events, respectively, in Super-Kamiokande. We…

High Energy Astrophysical Phenomena · Physics 2014-03-21 Ranjan Laha , John F. Beacom