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Related papers: Neutrino oscillations at dual baselines

200 papers

For the operation of precision neutrino experiments, the understanding of neutrino interactions with matter is a preconditioned requirement for all detections and measurements of neutrinos. The largest uncertainties in estimating…

High Energy Physics - Experiment · Physics 2025-01-16 Lars Bathe-Peters

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

Protvino to ORCA (Oscillation Research with Cosmics in the Abyss) (P2O) is an upcoming neutrino oscillation experiment with a very long baseline of 2595 km. Due to the substantial baseline, this experiment provides a unique opportunity to…

High Energy Physics - Phenomenology · Physics 2025-06-06 Chinmay Bera , K. N. Deepthi

In the last two decades the search for neutrinoless double beta decay has evolved into one of the highest priorities for understanding neutrinos and the origin of mass. The main reason for this paradigm shift has been the discovery of…

High Energy Physics - Experiment · Physics 2012-02-10 J. J. Gomez-Cadenas , J. Martin-Albo , M. Mezzetto , F. Monrabal , M. Sorel

Tokai to Kamioka (T2K) is a long-baseline neutrino oscillation experiment that measures oscillation parameters related to both $\nu_\mu(\bar{\nu}_\mu)$ disappearance and $\nu_e(\bar{\nu}_e)$ appearance in a $\nu_\mu(\bar{\nu}_\mu)$ beam.…

High Energy Physics - Experiment · Physics 2025-01-03 Michael Reh

To complete the picture of neutrino oscillations two fundamental parameters need to be measured, theta13 and delta. The next generation of long baseline neutrino oscillation experiments -superbeams, betabeams and neutrino factories- indeed…

High Energy Physics - Phenomenology · Physics 2009-11-11 J. Bernabeu , J. Burguet-Castell , C. Espinoza , M. Lindroos

This report provides the results of an extensive and important study of the potential for a U.S. scientific program that will extend our knowledge of neutrino oscillations well beyond what can be anticipated from ongoing and planned…

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

Light sterile neutrinos have been introduced as an explanation for a number of oscillation signals at $\Delta m^2 \sim 1$ eV$^2$. Neutrino oscillations at relatively short baselines provide a probe of these possible new states. This paper…

High Energy Physics - Phenomenology · Physics 2013-05-30 A. J. Anderson , J. M. Conrad , E. Figueroa-Feliciano , C. Ignarra , G. Karagiorgi , K. Scholberg , M. H. Shaevitz , J. Spitz

I give a brief overview of the physics potential of short baseline experiments at neutrino factories, i.e. facilities providing high energy and high intensity neutrino beams, like the one planned to be built in connection with the proposed…

High Energy Physics - Phenomenology · Physics 2009-10-31 Alexey A. Petrov

We consider possibilities of observing CP-violation effects in neutrino oscillation experiments with low energy ($\sim$ several hundreds MeV).

High Energy Physics - Phenomenology · Physics 2011-02-11 J. Sato

Future long-baseline experiments will play an important role in exploring physics beyond the standard model. One such new physics concept is the large extra dimension (LED), which provides an elegant solution to the hierarchy problem. This…

High Energy Physics - Phenomenology · Physics 2023-12-15 Samiran Roy

The next generation of long baseline neutrino experiments will aim at determining the value of the unknown mixing angle, theta_{13}, the type of neutrino mass hierarchy and the presence of CP-violation in the lepton sector. Beta-beams and…

High Energy Physics - Phenomenology · Physics 2009-06-19 J. Bernabeu , C. Espinoza , C. Orme , S. Palomares-Ruiz , S. Pascoli

We examine how large CP- and T-violation effects are allowed in long baseline neutrino experiments with three generations of neutrinos, considering both the solar neutrino deficit and the atmospheric neutrino anomaly. We considerd two…

High Energy Physics - Phenomenology · Physics 2008-02-03 Masafumi Koike , Joe Sato

Neutrino long-baseline experiments nowadays all use nuclear targets. The extraction of neutrino oscillation parameters from such experiments requires a good understanding of the interaction of neutrinos with nuclei. In this talk we discuss…

Nuclear Theory · Physics 2012-04-13 Ulrich Mosel , Olga Lalakulich

We discuss the physics potential of intermediate $L \sim 20 \div 30$ km baseline experiments at reactor facilities, assuming that the solar neutrino oscillation parameters $\Delta m^2_{\odot}$ and $\theta_{\odot}$ lie in the high-LMA…

High Energy Physics - Phenomenology · Physics 2011-02-11 Sandhya Choubey , S. T. Petcov , M. Piai

The KEK-to-Kamioka long-baseline neutrino experiment (K2K) has begun its investigation of neutrino oscillation, and has established the method of a long-baseline neutrino experiment. From the first 100 days of data-taking, a deficit of muon…

High Energy Physics - Experiment · Physics 2007-05-23 Takanobu Ishii

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

For neutrino oscillations to take place the entangled quantum state of a neutrino and a charged lepton produced via charged current interactions must be disentangled. Implementing a non-perturbative Wigner-Weisskopf method we obtain the…

High Energy Physics - Phenomenology · Physics 2011-09-05 Daniel Boyanovsky

Non-unitary neutrino mixing implies an extra CP violating phase that can fake the leptonic Dirac CP phase $\delta_{CP}$ of the simplest three-neutrino mixing benchmark scheme. This would hinder the possibility of probing for CP violation in…

High Energy Physics - Phenomenology · Physics 2017-03-03 Shao-Feng Ge , Pedro Pasquini , M. Tortola , J. W. F. Valle
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