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Multi-TeV muon colliders offer a powerful means of accessing new physics coupled to muons while generating clean and intense high-energy neutrino beams via muon decays. We study a fixed-target experiment leveraging the neutrino beams and a…

High Energy Physics - Phenomenology · Physics 2024-12-17 Hongkai Liu , Daiki Ueda

We report the measurements of single and double differential cross section of muon neutrino charged-current interactions on carbon with a single positively charged pion in the final state at the T2K off-axis near detector using…

High Energy Physics - Experiment · Physics 2020-01-29 K. Abe , R. Akutsu , A. Ali , C. Alt , J. Amey , C. Andreopoulos , L. Anthony , M. Antonova , S. Aoki , A. Ariga , Y. Ashida , E. T. Atkin , Y. Awataguchi , Y. Azuma , S. Ban , M. Barbi , G. J. Barker , G. Barr , C. Barry , M. Batkiewicz-Kwasniak , A. Beloshapkin , F. Bench , V. Berardi , S. Berkman , R. M. Berner , L. Berns , S. Bhadra , S. Bienstock , A. Blondel , S. Bolognesi , S. Bordoni , B. Bourguille , S. B. Boyd , D. Brailsford , A. Bravar , C. Bronner , M. Buizza Avanzini , J. Calcutt , R. G. Calland , T. Campbell , S. Cao , S. L. Cartwright , R. Castillo , M. G. Catanesi , A. Cervera , A. Chappell , C. Checchia , D. Cherdack , N. Chikuma , G. Christodoulou , J. Coleman , G. Collazuol , L. Cook , D. Coplowe , A. Cudd , A. Dabrowska , G. De Rosa , T. Dealtry , P. F. Denner , S. R. Dennis , C. Densham , F. Di Lodovico , N. Dokania , S. Dolan , O. Drapier , K. E. Duy , J. Dumarchez , P. Dunne , L. Eklund , S. Emery-Schrenk , A. Ereditato , P. Fernandez , T. Feusels , A. J. Finch , G. A. Fiorentini , G. Fiorillo , C. Francois , M. Friend , Y. Fujii , R. Fujita , D. Fukuda , R. Fukuda , Y. Fukuda , K. Gameil , A. Garcia , C. Giganti , F. Gizzarelli , T. Golan , M. Gonin , A. Gorin , M. Guigue , D. R. Hadley , L. Haegel , J. T. Haigh , P. Hamacher-Baumann , D. Hansen , J. Harada , M. Hartz , T. Hasegawa , N. C. Hastings , T. Hayashino , Y. Hayato , A. Hillairet , T. Hiraki , A. Hiramoto , S. Hirota , M. Hogan , J. Holeczek , N. T. Hong Van , F. Hosomi , K. Huang , F. Iacob , A. K. Ichikawa , M. Ikeda , J. Imber , T. Inoue , J. Insler , R. A. Intonti , T. Ishida , T. Ishii , M. Ishitsuka , E. Iwai , K. Iwamoto , A. Izmaylov , B. Jamieson , S. J. Jenkins , C. Jesus-Valls , M. Jiang , S. Johnson , P. Jonsson , C. K. Jung , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , D. Karlen , Y. Kataoka , T. Katori , Y. Kato , E. Kearns , M. Khabibullin , A. Khotjantsev , H. Kim , J. Kim , S. King , J. Kisiel , A. Knight , A. Knox , T. Kobayashi , L. Koch , T. Koga , P. P. Koller , A. Konaka , L. L. Kormos , Y. Koshio , K. Kowalik , H. Kubo , Y. Kudenko , N. Kukita , R. Kurjata , T. Kutter , M. Kuze , L. Labarga , J. Lagoda , I. Lamont , M. Lamoureux , P. Lasorak , M. Laveder , M. Lawe , M. Licciardi , T. Lindner , Z. J. Liptak , R. P. Litcheld , S. L. Liu , X. Li , A. Longhin , J. P. Lopez , T. Lou , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , M. Malek , S. Manly , L. Maret , A. D. Marino , J. F. Martin , P. Martins , S. Martynenko , T. Maruyama , T. Matsubara , K. Matsushita , V. Matveev , K. Mavrokoridis , W. Y. Ma , E. Mazzucato , M. McCarthy , N. McCauley , K. S. McFarland , C. McGrew , A. Mefodiev , C. Metelko , M. Mezzetto , A. Minamino , O. Mineev , S. Mine , A. Missert , M. Miura , L. Molina Bueno , S. Moriyama , J. Morrison , Th. A. Mueller , L. Munteanu , S. Murphy , Y. Nagai , T. Nakadaira , M. Nakahata , Y. Nakajima , A. Nakamura , K. G. Nakamura , K. Nakamura , K. D. Nakamura , Y. Nakanishi , S. Nakayama , T. Nakaya , K. Nakayoshi , C. Nantais , T. V. Ngoc , C. Nielsen , K. Niewczas , K. Nishikawa , Y. Nishimura , T. S. Nonnenmacher , F. Nova , P. Novella , J. Nowak , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , K. Okumura , T. Okusawa , W. Oryszczak , S. M. Oser T. Ovsyannikova , R. A. Owen , Y. Oyam , V. Palladino , J. L. Palomino , V. Paolone , W. C. Parker , N. D. Patel , P. Paudyal , M. Pavin , D. Payne , G. C. Penn , Y. Petrov L. Pickering , C. Pidcott , E. S. Pinzon Guerra , C. Pistillo , B. Popov K. Porwit , M. Posiadala-Zezula , J. M. Poutissou , A. Pritchard , P. Przewlocki , B. Quilain , T. Radermacher , E. Radicioni , B. Radics , P. N. Rato , M. A. Rayner , E. Reinherz-Aronis , C. Riccio , E. Rondio , B. Rossi , S. Roth , A. Rubbia , A. C. Ruggeri , A. Rychter , K. Sakashita , F. Sanchez , S. Sasaki , E. Scantamburlo , C. M. Schloesser , K. Scholberg , J. Schwehr , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , R. Shah , A. Shaikhiev , F. Shaker , D. Shaw , A. Shaykina , M. Shiozawa , T. Shirahige , W. Shorrock , A. Shvartsman , A. Smirnov , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , Y. Sonoda , J. Steinmann , T. Stewart , P. Stowell , Y. Suda , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , A. A. Sztuc , R. Tacik , M. Tada , A. Takeda , Y. Takeuchi , R. Tamura , H. K. Tanaka , H. A. Tanaka , S. Tanaka , T. Thakore , L. F. Thompson , S. Tobayama , W. Toki , T. Tomura , C. Touramanis , K. M. Tsui , T. Tsukamoto , M. Tzanov , Y. Uchida , W. Uno , M. Vagins , S. Valder , Z. Vallari , D. Vargas , G. Vasseur , C. Vilela , W. G. S. Vinning , T. Vladisavljevic , V. V. Volkov , T. Wachala , J. Walker , J. G. Walsh , C. W. Walter , Y. Wang , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , R. J. Wilson , K. Wood , C. Wret , Y. Yamada , K. Yamamoto , S. Yamasu , C. Yanagisawa , G. Yang , T. Yano , K. Yasutome , S. Yen , N. Yershov , M. Yokoyama , T. Yoshida , M. Yu , A. Zalewska , J. Zalipska , L. Zambelli , K. Zaremba , G. Zarnecki , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos , A. Zykova

The proposed KAON factory at the Triumf Laboratory in Vancouver, Canada provides a unique opportunity for high statistics long baseline neutrino oscillation experiments. Several possibilities are under active consideration. In this paper we…

High Energy Physics - Phenomenology · Physics 2008-02-03 Scott Hayward , Martin Sevior , Nathan Weiss , Dennis Wright

A new heavy gauge boson, W', decaying to a muon and a neutrino, is searched for in pp collisions at a centre-of-mass of 7 TeV. The data, collected with the CMS detector at the LHC, correspond to an integrated luminosity of 36 inverse…

High Energy Physics - Experiment · Physics 2015-05-27 CMS Collaboration

Many galactic and extragalactic astrophysical sources are currently considered promising candidates as high energy neutrino emitters. Astrophysical neutrinos can be detected as upward-going muons produced in charged-current interactions…

Astrophysics · Physics 2012-08-27 The MACRO Collaboration

We propose an explanation of the LSND evidence for electron antineutrino appearance based on neutrino decay. We introduce a heavy neutrino, which is produced in pion and muon decays because of a small mixing with muon neutrinos, and then…

High Energy Physics - Phenomenology · Physics 2009-11-11 Sergio Palomares-Ruiz , Silvia Pascoli , Thomas Schwetz

The neutrino produced in the pion decay reveals a new diffraction phenomenon due to many-body interactions in an intermediate time region when wave functions of the parent and daughters overlap. Because of diffraction, the probability to…

High Energy Physics - Phenomenology · Physics 2012-11-28 Kenzo Ishikawa , Yutaka Tobita

We discuss ways to explore non-standard interactions (NSI) which neutrinos may possess by expressing them as effective four Fermi operators with coefficient of the order of (M_{W} / M_{NP})^2 ~0.01 (0.0001) for energy scales of new physics…

High Energy Physics - Phenomenology · Physics 2008-05-19 Hisakazu Minakata

We calculate event rate and demonstrate the observational feasibility of very high energy muons (1-1000 TeV) in a large mass underground detector operating as a pair-meter. This energy range corresponds to surface muon energies of $\sim$(5…

High Energy Physics - Phenomenology · Physics 2009-11-11 Raj Gandhi , Sukanta Panda

The search strategy or the finding of new effects for heavy neutrinos often relies on their different decay channels to detectable particles. In particular in this work we study the decay of a Majorana neutrino with interactions obtained…

High Energy Physics - Phenomenology · Physics 2015-12-02 Lucia Duarte , Javier Peressutti , O. A. Sampayo

The sensitivity of beam dump experiments to heavy neutrinos depends on the relative size of their mixings with the lepton flavours in the Standard Model. We study the impact of present neutrino oscillation data on these mixing angles in the…

High Energy Physics - Phenomenology · Physics 2020-11-23 Marco Drewes , Jan Hajer , Juraj Klaric , Gaia Lanfranchi

A very massive star with a carbon-oxygen core in the range of $64$ M$_{\odot}<M_{\mathrm{CO}}<133$ M$_{\odot}$ is expected to undergo a very different kind of explosion known as a pair instability supernova. Pair instability supernovae are…

High Energy Astrophysical Phenomena · Physics 2017-11-22 Warren P. Wright , Matthew S. Gilmer , Carla Fröhlich , James P. Kneller

The physics potential of an intense source of low-energy muons is studied. Such a source is a necessary stage towards building the neutrino factories and muon colliders which are being considered at present. The CERN Neutrino Factory could…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Aysto , A. Baldini , A. Blondel , A. de Gouvea , J. Ellis , W. Fetscher , G. F. Giudice , K. Jungmann , S. Lola , V. Palladino , K. Tobe , A. Vacchi , A. van der Schaaf , K. Zuber

As measurements of the neutrino oscillation parameters improve it is becoming more interesting to study antineutrino oscillations, to investigate CP and CPT violation in the lepton sector and nonstandard matter effects. We present the most…

High Energy Physics - Experiment · Physics 2016-07-13 Kirsty Duffy

The theory of neutrino oscillation predicts that if both neutrino and antineutrino coming from $Z_0$ decay are detected, one can observe an oscillation pattern between the corresponding detectors. This prediction is based on two properties;…

High Energy Physics - Phenomenology · Physics 2023-01-19 M. M. Ettefaghi , Z. Askaripour Ravari

A muon collider is expected to produce a high intensity neutrino beam which is an admixture of either $\nu_{\mu}+\bar{\nu_e}$ or $\bar{\nu}_{\mu} +\nu_e$ which can can be directed to underground detectors far away from the source. It will…

High Energy Physics - Phenomenology · Physics 2011-07-19 R. N. Mohapatra

We calculate the signal rate of hypothetical heavy neutral leptons (HNL or sterile neutrinos) from kaon decays expected in the framework of the SHiP experiment. The kaons are produced in the hadronic shower initiated in the beam-dump mode…

High Energy Physics - Phenomenology · Physics 2020-10-20 Dmitry Gorbunov , Igor Krasnov , Yury Kudenko , Sergey Suvorov

Sterile neutrinos are SU(2) singlets that mix with active neutrinos via a mass matrix, its diagonalization leads to mass eigenstates that couple via standard model vertices. We study the cosmological production of heavy neutrinos via…

Cosmology and Nongalactic Astrophysics · Physics 2016-06-15 Louis Lello , Daniel Boyanovsky

We investigate the present constraints from MINOS and T2K experiments for the neutrino decay scenario induced by non-diagonal couplings of Majorons to neutrinos. As novelty, on top of the typical invisible decay prescription, we add the…

High Energy Physics - Phenomenology · Physics 2017-12-06 Alberto M. Gago , Ricardo A. Gomes , Abner L. G. Gomes , Joel Jones-Perez , Orlando L. G. Peres

T2K is a long-baseline neutrino oscillation experiment using a $\nu_{\mu}$ beam produced at the J-PARC facility. Neutrinos are detected at a Near Detector complex (ND280) and at the Far Detector (Super-Kamiokande). The most recent…

High Energy Physics - Experiment · Physics 2018-04-02 Claudio Giganti
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