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The hydrogen-like muonium atom ($\mu^+e^-$) consists of a positive muon ($\mu^+$) and an electron ($e^-$). Since it was first observed by Hughes et al. in 1960, a series of precision experiments could be carried out testing bound state…

Atomic Physics · Physics 2016-09-08 K. Jungmann

A very compact architecture has been developed for the first level Muon Trigger of the LHCb experiment that processes 40 millions of proton-proton collisions per second. For each collision, it receives 3.2 kBytes of data and it finds…

In a neutron lifetime experiment conducted at the National Institute of Standards and Technology, protons produced by neutron decay events are confined in a Penning trap. In each run of the experiment, there is a trapping stage of duration…

Data Analysis, Statistics and Probability · Physics 2008-11-26 Kevin J. Coakley

Precision measurements in nuclear muon capture on the proton and $^3$He allow for tests of the Standard Model for the strong and electroweak interactions, complementary to those achieved in high energy experiments. The present situation and…

High Energy Physics - Phenomenology · Physics 2009-10-31 Jan Govaerts

The potentiality of an experiment measuring the muon polarization in $K^+\rightarrow\pi^0\mu^+\nu_\mu$ at a $\phi$ factory is discussed, with particular attention to the possibility of revealing unexpected violation of Time reversal…

High Energy Physics - Phenomenology · Physics 2007-05-23 Paolo Privitera

Next generation low-background experiments require a detailed understanding of all possible radiation backgrounds. One important radiation source are muon-induced neutrons. Their production processes are up to now not fully understood. New…

Instrumentation and Detectors · Physics 2019-04-04 R. Kneißl , A. Caldwell , Q. Du , A. Empl , C. Gooch , X. Liu , B. Majorovits , M. Palermo , O. Schulz

In recent neutrino detectors, neutrons produced in neutrino reactions play an important role. Muon capture on oxygen nuclei is one of the processes that produce neutrons in water Cherenkov detectors. We measured neutron multiplicity in the…

High Energy Physics - Experiment · Physics 2026-04-02 Kamiokande Collaboration , S. Miki , 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. Mine , M. Miura , S. Moriyama , M. Nakahata , S. Nakayama , Y. Noguchi , K. Okamoto , G. Pronost , K. Sato , H. Sekiya , H. Shiba , K. Shimizu , M. Shiozawa , Y. Sonoda , Y. Suzuki , A. Takeda , Y. Takemoto , A. Takenaka , H. Tanaka , S. Watanabe , T. Yano , T. Kajita , K. Okumura , T. Tashiro , T. Tomiya , X. Wang , S. Yoshida , G. D. Megias , P. Fernandez , L. Labarga , N. Ospina , B. Zaldivar , B. W. Pointon , C. Yanagisawa , E. Kearns , J. L. Raaf , L. Wan , T. Wester , J. Bian , B. Cortez , N. J. Griskevich , S. Locke , 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. Ershova , A. Giampaolo , Th. A. Mueller , A. D. Santos , P. Paganini , C. Quach , B. Quilain , R. Rogly , T. Nakamura , J. S. Jang , R. P. Litchfield , L. N. Machado , F. J. P. Soler , J. G. Learned , K. Choi , N. Iovine , S. Cao , L. H. V. Anthony , D. Martin , N. W. Prouse , M. Scott , A. A. Sztuc , Y. Uchida , V. Berardi , N. F. Calabria , M. G. Catanesi , E. Radicioni , N. F. Calabria , A. Langella , G. De Rosa , G. Collazuol , M. Feltre , F. Iacob , M. Lamoureux , M. Mattiazzi , L. Ludovici , M. Gonin , L. Périssé , B. Quilain , C. Fujisawa , S. Horiuchi , 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 , Y. Kotsar , H. Ozaki , A. T. Suzuki , Y. Takagi , Y. Takeuchi , H. Zhong , J. Feng , L. Feng , S. Han , 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 , P. Mehta , A. Tarrant , M. J. Wilking , Y. Fukuda , Y. Itow , H. Menjo , K. Ninomiya , Y. Yoshioka , J. Lagoda , M. Mandal , P. Mijakowski , Y. S. Prabhu , J. Zalipska , M. Jia , J. Jiang , C. K. Jung , W. Shi , M. J. Wilking , Y. Hino , H. Ishino , H. Kitagawa , 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 , B. S. Yang , 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 , 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 , T. Kinoshita , Y. Ommura , N. Shigeta , M. Shinoki , T. Suganuma , K. Yamauchi , T. Yoshida , J. F. Martin , H. A. Tanaka , T. Towstego , 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 , A. Minamino , G. Pintaudi , S. Sano , R. Shibayama , R. Shimamura , S. Suzuki , K. Wada

The Mu2e experiment will search for a Standard Model violating rate of neutrinoless conversion of a muon into an electron in the presence of an aluminum nucleus. Observation of this charged lepton flavor violating process would be an…

High Energy Physics - Experiment · Physics 2022-10-28 Michael Thomas Hedges

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 designed a simple setup to measure the muon lifetime and the electron energy spectra of muon decay. A low cost coincidental circuit was designed to select the signals of muon decay events detected by a plastic scintillator detector. It…

Instrumentation and Detectors · Physics 2016-08-26 Yushi Hu , Tianye Wang , Yefeng Mei , Zhao Zhang , Chuangang Ning

The next generation of "intensity frontier" facilities will bring a significant increase in the intensity of sub-relativistic beams of $\mu^-$. We show that the use of these beams in combination with thin targets of $Z\sim 30$ elements…

High Energy Physics - Phenomenology · Physics 2012-07-03 David McKeen , Maxim Pospelov

The AlCap experiment is a joint venture between the COMET and Mu2e collaborations that will measure the rate and spectrum of particles emitted after nuclear muon capture on aluminium. Both collaborations will search for the charged lepton…

Instrumentation and Detectors · Physics 2018-09-27 Andrew Edmonds

The recent discovery of the Higgs particle of 125 GeV has revised the interest of the so-called Higgs factory, namely of a mu+mu- collider with adequately cooled intensity of about 6 10^12 muons of each sign, a repetition rate of 15-50 p/s…

Accelerator Physics · Physics 2013-09-02 Carlo Rubbia

Recent results of an aging test performed at the CERN Gamma Irradiation Facility on a single--gap RPC prototype developed for the LHCb Muon System are presented. The results are based on an accumulated charge of about 0.45 C/cm$^2$,…

We show that ordinary and radiative muon capture impose stringent constraints on sterile neutrino properties. In particular, we consider a sterile neutrino with a mass between 40 to $80 {\rm MeV}$ that has a large mixing with the muon…

High Energy Physics - Phenomenology · Physics 2011-01-12 David McKeen , Maxim Pospelov

We report a measurement of muon annual modulation in a 12-liter liquid scintillation detector with a live-time of more than 4 years at the Soudan Underground Laboratory. Muon minimum ionization in the detector is identified by its observed…

High Energy Physics - Experiment · Physics 2019-10-23 C. Zhang , D. -M. Mei

It has been very recently reported (McKeen, Pospelov, arXive:1011.3046) that the parameter region suggested for an explanation of the neutrino oscillation results from the LSND, KARMEN and MiniBooNE experiments in terms of the production…

High Energy Physics - Phenomenology · Physics 2010-11-29 S. N. Gninenko

Experimental and theoretical activities are underway at CERN with the aim of examining the feasibility of a very-high-flux neutrino source. In the present scheme, a high-power proton beam (some 4 MW) bombards a target where pions are…

Accelerator Physics · Physics 2014-11-18 G. Franchetti , S. Gilardoni , P. Gruber , K. Hanke , H. Haseroth , E. B. Holzer , D. Kuechler , A. M. Lombardi , R. Scrivens

We describe the data acquisition system for the MuLan muon lifetime experiment at Paul Scherrer Institute. The system was designed to record muon decays at rates up to 1 MHz and acquire data at rates up to 60 MB/sec. The system employed a…

The neutron lifetime, $\tau$ = 880.2 $\pm$ 1.0 sec , is an important parameter for particle physics and cosmology. There is, however, an 8.4 sec (4.0$\,\sigma$) deviation between the measured value of the neutron lifetime using two methods…

Instrumentation and Detectors · Physics 2018-12-26 Naoyuki Sumi , Hidetoshi Otono , Tamaki Yoshioka , Kenji Mishima , Yasuhiro Makida
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