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The SHiP experiment is designed to search for very weakly interacting particles beyond the Standard Model which are produced in a 400 GeV/c proton beam dump at the CERN SPS. An essential task for the experiment is to keep the Standard Model…

Instrumentation and Detectors · Physics 2017-05-19 SHiP collaboration , A. Akmete , A. Alexandrov , A. Anokhina , S. Aoki , E. Atkin , N. Azorskiy , J. J. Back , A. Bagulya , A. Baranov , G. J. Barker , A. Bay , V. Bayliss , G. Bencivenni , A. Y. Berdnikov , Y. A. Berdnikov , M. Bertani , C. Betancourt , I. Bezshyiko , O. Bezshyyko , D. Bick , S. Bieschke , A. Blanco , J. Boehm , M. Bogomilov , K. Bondarenko , W. M. Bonivento , A. Boyarsky , R. Brenner , D. Breton , R. Brundler , M. Bruschi , V. Büscher , A. Buonaura , S. Buontempo , S. Cadeddu , A. Calcaterra , M. Campanelli , J. Chauveau , A. Chepurnov , M. Chernyavsky , K. -Y. Choi , A. Chumakov , P. Ciambrone , G. M. Dallavalle , N. D'Ambrosio , G. D'Appollonio , G. De Lellis , A. De Roeck , M. De Serio , L. Dedenko , A. Di Crescenzo , N. Di Marco , C. Dib , H. Dijkstra , V. Dmitrenko , D. Domenici , S. Donskov , A. Dubreuil , J. Ebert , T. Enik , A. Etenko , F. Fabbri , L. Fabbri , O. Fedin , G. Fedorova , G. Felici , M. Ferro-Luzzi , R. A. Fini , P. Fonte , C. Franco , T. Fukuda , G. Galati , G. Gavrilov , S. Gerlach , L. Golinka-Bezshyyko , D. Golubkov , A. Golutvin , D. Gorbunov , S. Gorbunov , V. Gorkavenko , Y. Gornushkin , M. Gorshenkov , V. Grachev , E. Graverini , V. Grichine , A. M. Guler , Yu. Guz , C. Hagner , H. Hakobyan , E. van Herwijnen , A. Hollnagel , B. Hosseini , M. Hushchyn , G. Iaselli , A. Iuliano , R. Jacobsson , M. Jonker , I. Kadenko , C. Kamiscioglu , M. Kamiscioglu , M. Khabibullin , G. Khaustov , A. Khotyantsev , S. H. Kim , V. Kim , Y. G. Kim , N. Kitagawa , J. -W. Ko , K. Kodama , A. Kolesnikov , D. I. Kolev , V. Kolosov , M. Komatsu , N. Konovalova , M. A. Korkmaz , I. Korol , I. Korol'ko , A. Korzenev , S. Kovalenko , I. Krasilnikova , K. Krivova , Y. Kudenko , V. Kurochka , E. Kuznetsova , H. M. Lacker , A. Lai , G. Lanfranchi , O. Lantwin , A. Lauria , H. Lebbolo , K. Y. Lee , J. -M. Lévy , V. Likacheva , L. Lopes , V. Lyubovitskij , J. Maalmi , A. Magnan , V. Maleev , A. Malinin , A. Mefodev , P. Mermod , S. Mikado , Yu. Mikhaylov , D. A. Milstead , O. Mineev , A. Montanari , M. C. Montesi , K. Morishima , S. Movchan , N. Naganawa , M. Nakamura , T. Nakano , A. Novikov , B. Obinyakov , S. Ogawa , N. Okateva , P. H. Owen , A. Paoloni , B. D. Park , L. Paparella , A. Pastore , M. Patel , D. Pereyma , D. Petrenko , K. Petridis , D. Podgrudkov , V. Poliakov , N. Polukhina , M. Prokudin , A. Prota , A. Rademakers , F. Ratnikov , T. Rawlings , M. Razeti , F. Redi , S. Ricciardi , T. Roganova , A. Rogozhnikov , H. Rokujo , G. Rosa , T. Rovelli , O. Ruchayskiy , T. Ruf , V. Samoylenko , A. Saputi , O. Sato , E. S. Savchenko , W. Schmidt-Parzefall , N. Serra , A. Shakin , M. Shaposhnikov , P. Shatalov , T. Shchedrina , L. Shchutska , V. Shevchenko , H. Shibuya , A. Shustov , S. B. Silverstein , S. Simone , M. Skorokhvatov , S. Smirnov , J. Y. Sohn , A. Sokolenko , N. Starkov , B. Storaci , P. Strolin , S. Takahashi , I. Timiryasov , V. Tioukov , N. Tosi , D. Treille , R. Tsenov , S. Ulin , A. Ustyuzhanin , Z. Uteshev , G. Vankova-Kirilova , F. Vannucci , P. Venkova , S. Vilchinski , M. Villa , K. Vlasik , A. Volkov , R. Voronkov , R. Wanke , J. -K. Woo , M. Wurm , S. Xella , D. Yilmaz , A. U. Yilmazer , C. S. Yoon , Yu. Zaytsev

We investigate novel strategies to extend the sensitivity of dark matter direct detection experiments to energy deposits well below the thresholds of conventional detectors. In liquid-argon time-projection chambers equipped with silicon…

Instrumentation and Detectors · Physics 2026-01-12 Faeq Abed , Asmaa AlMellah , Kareem Al-Jubouri , Alex Lumoski

A short summary of the LHCb muon identification procedure is given in this article. First, the muon system of LHCb is presented, together with some examples of physics measurements of the experiment where the muon identification is crucial.…

High Energy Physics - Experiment · Physics 2010-05-17 X. Cid Vidal

We studied the ionization of hydrogen by scattering of neutrino magnetic moment, relativistic muon, and weakly-interacting massive particle with a QED-like interaction. Analytic results were obtained and compared with several approximation…

High Energy Physics - Phenomenology · Physics 2013-08-28 Jiunn-Wei Chen , C. -P. Liu , Chien-Fu Liu , Chih-Liang Wu

Since its discovery in the 1930s, the muon has played an important role in our quest to understand the sub-atomic theory of matter. The muon was the first second-generation standard-model particle to be discovered, and its decay has…

High Energy Physics - Experiment · Physics 2008-11-26 B. Lee Roberts

The monoenergetic 236 MeV muon neutrino from charged kaon decay-at-rest ($K^+ \rightarrow \mu^+ \nu_\mu$) can be used to produce a novel set of cross section measurements. Applicable for short- and long-baseline accelerator-based neutrino…

Instrumentation and Detectors · Physics 2014-05-20 J. Spitz

Dark photons are predicted by various new physics models, and are being intensively studied in a variety of experiments. In the first part of this paper, we obtain partial wave unitarity constraints on the dark photon parameter space from…

High Energy Physics - Phenomenology · Physics 2024-10-25 Yasaman Hosseini , Mojtaba Mohammadi Najafabadi

The Mu2e experiment will search for the charged-lepton flavor violating (CLFV) neutrino-less conversion of a negative muon into an electron in the field of a nucleus. The conversion process results in a monochromatic electron with an energy…

Instrumentation and Detectors · Physics 2019-02-01 R. H. Bernstein

Muon catalyzed fusion in deuterium has traditionally been studied in gaseous and liquid targets. The TRIUMF solid-hydrogen-layer target system has been used to study the fusion reaction rates in the solid phase of D_2 at a target…

A preliminary analysis is presented of low-energy ($\bar{E_\nu} \sim 4 GeV$) neutrino interactions observed by the MACRO detector. These include neutrino interactions in the detector, as well as upgoing neutrino-induced muons that stop in…

High Energy Physics - Experiment · Physics 2019-08-14 R. Nolty

The Muon g-2/EDM Experiment at J-PARC will employ a novel way to measure the muon magnetic anomaly, a_mu = (g-2)_mu/2, by using a low-emittance beam of positive muons stored in a compact muon storage magnet. The experimental method includes…

High Energy Physics - Experiment · Physics 2025-12-24 Graziano Venanzoni

With no concrete evidence for non-gravitational interactions of dark matter to date, it is natural to wonder whether dark matter couples predominantly to the Standard Model (SM)'s neutrinos. Neutrino interactions (and the possible existence…

High Energy Physics - Phenomenology · Physics 2025-05-20 Jyotismita Adhikary , Kevin J. Kelly , Felix Kling , Sebastian Trojanowski

The possibility to observe the neutrino-less double $ \beta $ decay and thus to prove the Majorana nature of neutrino as well as provide a sensitive measure of its mass is a major challenge of to-day's neutrino physics. As an attractive…

High Energy Physics - Phenomenology · Physics 2009-11-10 Z. Sujkowski , S. Wycech

The low energy radiative capture process n+p -> d+gamma provides a sensitive probe of the two-nucleon system. The cross section for this process is dominated by the isovector M1 amplitude for capture from the 1S0 channel via the isovector…

Nuclear Theory · Physics 2009-10-31 Jiunn-Wei Chen , Gautam Rupak , Martin J. Savage

High-energy cosmic rays are observed indirectly by detecting the extensive air showers initiated in Earth's atmosphere. The interpretation of experimental data relies on accurate modeling of the air shower development. Simulations based on…

High Energy Astrophysical Phenomena · Physics 2025-09-23 Lilly Pyras , Dennis Soldin , Felix Riehn

Muon colliders and neutrino factories are attractive options for future facilities aimed at achieving the highest lepton-antilepton collision energies and precision measurements of Higgs boson and neutrino mixing matrix parameters. The…

Accelerator Physics · Physics 2019-08-14 Daniel M. Kaplan

Muon colliders offer the possibility to go to very high energies with relatively small circular colliders, energies up to 10 or 14 TeV are envisioned. Due to their very clean collider environment they provide a fantastic tool to search for…

High Energy Physics - Phenomenology · Physics 2023-05-23 Jürgen Reuter

The complete 5.4 kton MINOS far detector has been taking data since the beginning of August 2003 at a depth of 2070 meters water-equivalent in the Soudan mine, Minnesota. This paper presents the first MINOS observations of muon neutrino and…

High Energy Physics - Experiment · Physics 2012-08-27 MINOS Collaboration

The production of a mu+mu- pair from the scattering of a muon-neutrino off the Coulomb field of a nucleus, known as neutrino trident production, is a sub-weak process that has been observed in only a couple of experiments. As such, we show…

High Energy Physics - Phenomenology · Physics 2014-09-05 Wolfgang Altmannshofer , Stefania Gori , Maxim Pospelov , Itay Yavin
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