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We present a momentum measurement method based on multiple Coulomb scattering (MCS) in the FASER$\nu$ emulsion detector. The measurement of charged-particle momenta is essential for studying neutrino interactions in the TeV energy range at…

Instrumentation and Detectors · Physics 2026-02-20 FASER Collaboration , Roshan Mammen Abraham , Xiaocong Ai , Saul Alonso Monsalve , John Anders , Emma Kate Anderson , Claire Antel , Akitaka Ariga , Tomoko Ariga , Jeremy Atkinson , Florian U. Bernlochner , Tobias Boeckh , Eliot Bornand , Jamie Boyd , Lydia Brenner , Angela Burger , Franck Cadoux , Roberto Cardella , David W. Casper , Charlotte Cavanagh , Shiyang Chen , Xin Chen , Xing Cheng , Kohei Chinone , Dhruv Chouhan , Andrea Coccaro , Stephane Débieux , Ansh Desai , Sergey Dmitrievsky , Radu Dobre , Monica D'Onofrio , Sinead Eley , Yannick Favre , Jonathan L. Feng , Carlo Alberto Fenoglio , Didier Ferrere , Max Fieg , Wissal Filali , Elena Firu , Haruhi Fujimori , Edward Galantay , Ali Garabaglu , Stephen Gibson , Sergio Gonzalez-Sevilla , Yuri Gornushkin , Yotam Granov , Jinjing Gu , Carl Gwilliam , Elie Hammou , Daiki Hayakawa , Michael Holzbock , Shih-Chieh Hsu , Zhen Hu , Giuseppe Iacobucci , Tomohiro Inada , Luca Iodice , Sune Jakobsen , Cesar Jesus-Valls , Arash Jofrehei , Hans Joos , Enrique Kajomovitz , Takumi Kanai , Hiroaki Kawahara , Alex Keyken , Felix Kling , Daniela Köck , Pantelis Kontaxakis , Jelle Koorn , Umut Kose , Peter Krack , Susanne Kuehn , Thanushan Kugathasan , Sebastian Laudage , Lorne Levinson , Botao Li , Jinfeng Liu , Yi Liu , Margaret S. Lutz , Jack MacDonald , Joern Mahlstedt , Toni Mäkelä , Anna Mascellani , Lawson McCoy , Josh McFayden , Andrea Pizarro Medina , Théo Moretti , Keiko Moriyama , Toshiyuki Nakano , Laurie Nevay , Motoya Nonaka , Yuma Ohara , Ken Ohashi , Kazuaki Okui , Hidetoshi Otono , Lorenzo Paolozzi , Annabelle Parry , Pawan Pawan , Brian Petersen , Titi Preda , Markus Prim , Junkai Qin , Michaela Queitsch-Maitland , Juan Rojo , Hiroki Rokujo , André Rubbia , Osamu Sato , Paola Scampoli , Kristof Schmieden , Matthias Schott , Cristiano Sebastiani , Anna Sfyrla , Davide Sgalaberna , Mansoora Shamim , Yosuke Takubo , Noshin Tarannum , Simon Thor , Eric Torrence , Oscar Ivan Valdes Martinez , Svetlana Vasina , Benedikt Vormwald , Chi Wang , Yuxiao Wang , Eli Welch , Aaron White , Monika Wielers , Benjamin James Wilson , Yue Xu , Heng Yang , Lekai Yao , Daichi Yoshikawa , Stefano Zambito , Shunliang Zhang , Yuxuan Zhang , Xingyu Zhao , Zijian Zhao

We present and analyze QCD corrections to the baryon magnetic moments in terms of the one-, two-, and three-body operators which appear in the effective field theory developed in our recent papers. The main corrections are extended…

High Energy Physics - Phenomenology · Physics 2009-11-07 Phuoc Ha , Loyal Durand

The upcoming MUonE experiment aims to precisely measure the running of the fine structure constant via elastic muon-electron scattering, to shed light on the current tension in the muon's anomalous magnetic moment. In addition to its…

High Energy Physics - Phenomenology · Physics 2025-11-06 Duncan Rocha , Isaac R. Wang

The muon g-2 experiment at Brookhaven National Laboratory measures the anomalous magnetic moment of the muon, $a_\mu$, very precisely. This measurement tests the Standard Model. The analysis for the data collected in 2000 (a $\mu^+$ run) is…

High Energy Physics - Experiment · Physics 2019-08-14 Cenap S. Ozben

Some recent precision experiments in low energy muon physics are discussed. Spectroscopy on the muonium atom, the bound state of a positve muon and an electron, has provided precise tests of standard theory and yielded most precise values…

Nuclear Experiment · Physics 2016-09-08 Klaus P. Jungmann

The aim of the MuCap experiment is a 1% measurement of the singlet capture rate Lambda_S for the basic electro-weak reaction mu + p -> n + nu_mu. This observable is sensitive to the weak form-factors of the nucleon, in particular to the…

The forward-backward charge asymmetry for the process $q\bar{q} \rightarrow Z/\gamma^{\ast} \rightarrow \mu^{+}\mu^{-}$ is measured as a function of the invariant mass of the dimuon system. Measurements are performed using proton proton…

High Energy Physics - Experiment · Physics 2015-12-17 LHCb collaboration , R. Aaij , B. Adeva , M. Adinolfi , A. Affolder , Z. Ajaltouni , S. Akar , J. Albrecht , F. Alessio , M. Alexander , S. Ali , G. Alkhazov , P. Alvarez Cartelle , A. A. Alves , S. Amato , S. Amerio , Y. Amhis , L. An , L. Anderlini , J. Anderson , G. Andreassi , M. Andreotti , J. E. Andrews , R. B. Appleby , O. Aquines Gutierrez , F. Archilli , P. d'Argent , A. Artamonov , M. Artuso , E. Aslanides , G. Auriemma , M. Baalouch , S. Bachmann , J. J. Back , A. Badalov , C. Baesso , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , W. Barter , V. Batozskaya , V. Battista , A. Bay , L. Beaucourt , J. Beddow , F. Bedeschi , I. Bediaga , L. J. Bel , V. Bellee , N. Belloli , I. Belyaev , E. Ben-Haim , G. Bencivenni , S. Benson , J. Benton , A. Berezhnoy , R. Bernet , A. Bertolin , M. -O. Bettler , M. van Beuzekom , A. Bien , S. Bifani , P. Billoir , T. Bird , A. Birnkraut , A. Bizzeti , T. Blake , F. Blanc , J. Blouw , S. Blusk , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , M. Borsato , T. J. V. Bowcock , E. Bowen , C. Bozzi , S. Braun , M. Britsch , T. Britton , J. Brodzicka , N. H. Brook , E. Buchanan , A. Bursche , J. Buytaert , S. Cadeddu , R. Calabrese , M. Calvi , M. Calvo Gomez , P. Campana , D. Campora Perez , L. Capriotti , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , P. Carniti , L. Carson , K. Carvalho Akiba , G. Casse , L. Cassina , L. Castillo Garcia , M. Cattaneo , Ch. Cauet , G. Cavallero , R. Cenci , M. Charles , Ph. Charpentier , M. Chefdeville , S. Chen , S. -F. Cheung , N. Chiapolini , M. Chrzaszcz , X. Cid Vidal , G. Ciezarek , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , V. Coco , J. Cogan , E. Cogneras , V. Cogoni , L. Cojocariu , G. Collazuol , P. Collins , A. Comerma-Montells , A. Contu , A. Cook , M. Coombes , S. Coquereau , G. Corti , M. Corvo , B. Couturier , G. A. Cowan , D. C. Craik , A. Crocombe , M. Cruz Torres , S. Cunliffe , R. Currie , C. D'Ambrosio , E. Dall'Occo , J. Dalseno , P. N. Y. David , A. Davis , O. De Aguiar Francisco , K. De Bruyn , S. De Capua , M. De Cian , J. M. De Miranda , L. De Paula , P. De Simone , C. -T. Dean , D. Decamp , M. Deckenhoff , L. Del Buono , N. Déléage , M. Demmer , D. Derkach , O. Deschamps , F. Dettori , B. Dey , A. Di Canto , F. Di Ruscio , H. Dijkstra , S. Donleavy , F. Dordei , M. Dorigo , A. Dosil Suárez , D. Dossett , A. Dovbnya , K. Dreimanis , L. Dufour , G. Dujany , F. Dupertuis , P. Durante , R. Dzhelyadin , A. Dziurda , A. Dzyuba , S. Easo , U. Egede , V. Egorychev , S. Eidelman , S. Eisenhardt , U. Eitschberger , R. Ekelhof , L. Eklund , I. El Rifai , Ch. Elsasser , S. Ely , S. Esen , H. M. Evans , T. Evans , A. Falabella , C. Färber , N. Farley , S. Farry , R. Fay , D. Ferguson , V. Fernandez Albor , F. Ferrari , F. Ferreira Rodrigues , M. Ferro-Luzzi , S. Filippov , M. Fiore , M. Fiorini , M. Firlej , C. Fitzpatrick , T. Fiutowski , K. Fohl , P. Fol , M. Fontana , F. Fontanelli , R. Forty , M. Frank , C. Frei , M. Frosini , J. Fu , E. Furfaro , A. Gallas Torreira , D. Galli , S. Gallorini , S. Gambetta , M. Gandelman , P. Gandini , Y. Gao , J. García Pardiñas , J. Garra Tico , L. Garrido , D. Gascon , C. Gaspar , R. Gauld , L. Gavardi , G. Gazzoni , D. Gerick , E. Gersabeck , M. Gersabeck , T. Gershon , Ph. Ghez , S. Gianì , V. Gibson , O. G. Girard , L. Giubega , V. V. Gligorov , C. Göbel , D. Golubkov , A. Golutvin , A. Gomes , C. Gotti , M. Grabalosa Gándara , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , E. Graverini , G. Graziani , A. Grecu , E. Greening , S. Gregson , P. Griffith , L. Grillo , O. Grünberg , B. Gui , E. Gushchin , Yu. Guz , T. Gys , T. Hadavizadeh , C. Hadjivasiliou , G. Haefeli , C. Haen , S. C. Haines , S. Hall , B. Hamilton , X. Han , S. Hansmann-Menzemer , N. Harnew , S. T. Harnew , J. Harrison , J. He , T. Head , V. Heijne , K. Hennessy , P. Henrard , L. Henry , E. van Herwijnen , M. Heß , A. Hicheur , D. Hill , M. Hoballah , C. Hombach , W. Hulsbergen , T. Humair , N. Hussain , D. Hutchcroft , D. Hynds , M. Idzik , P. Ilten , R. Jacobsson , A. Jaeger , J. Jalocha , E. Jans , A. Jawahery , F. Jing , M. John , D. Johnson , C. R. Jones , C. Joram , B. Jost , N. Jurik , S. Kandybei , W. Kanso , M. Karacson , T. M. Karbach , S. Karodia , M. Kecke , M. Kelsey , I. R. Kenyon , M. Kenzie , T. Ketel , E. Khairullin , B. Khanji , C. Khurewathanakul , S. Klaver , K. Klimaszewski , O. Kochebina , M. Kolpin , I. Komarov , R. F. Koopman , P. Koppenburg , M. Kozeiha , L. Kravchuk , K. Kreplin , M. Kreps , G. Krocker , P. Krokovny , F. Kruse , W. Krzemien , W. Kucewicz , M. Kucharczyk , V. Kudryavtsev , A. K. Kuonen , K. Kurek , T. Kvaratskheliya , D. Lacarrere , G. Lafferty , A. Lai , D. Lambert , G. Lanfranchi , C. Langenbruch , B. Langhans , T. Latham , C. Lazzeroni , R. Le Gac , J. van Leerdam , J. -P. Lees , R. Lefèvre , A. Leflat , J. Lefrançois , E. Lemos Cid , O. Leroy , T. Lesiak , B. Leverington , Y. Li , T. Likhomanenko , M. Liles , R. Lindner , C. Linn , F. Lionetto , B. Liu , X. Liu , D. Loh , I. Longstaff , J. H. Lopes , D. Lucchesi , M. Lucio Martinez , H. Luo , A. Lupato , E. Luppi , O. Lupton , A. Lusiani , F. Machefert , F. Maciuc , O. Maev , K. Maguire , S. Malde , A. Malinin , G. Manca , G. Mancinelli , P. Manning , A. Mapelli , J. Maratas , J. F. Marchand , U. Marconi , C. Marin Benito , P. Marino , J. Marks , G. Martellotti , M. Martin , M. Martinelli , D. Martinez Santos , F. Martinez Vidal , D. Martins Tostes , A. Massafferri , R. Matev , A. Mathad , Z. Mathe , C. Matteuzzi , A. Mauri , B. Maurin , A. Mazurov , M. McCann , J. McCarthy , A. McNab , R. McNulty , B. Meadows , F. Meier , M. Meissner , D. Melnychuk , M. Merk , E Michielin , D. A. Milanes , M. -N. Minard , D. S. Mitzel , J. Molina Rodriguez , I. A. Monroy , S. Monteil , M. Morandin , P. Morawski , A. Mordà , M. J. Morello , J. Moron , A. B. Morris , R. Mountain , F. Muheim , D. Müller , J. Müller , K. Müller , V. Müller , M. Mussini , B. Muster , P. Naik , T. Nakada , R. Nandakumar , A. Nandi , I. Nasteva , M. Needham , N. Neri , S. Neubert , N. Neufeld , M. Neuner , A. D. Nguyen , T. D. Nguyen , C. Nguyen-Mau , V. Niess , R. Niet , N. Nikitin , T. Nikodem , A. Novoselov , D. P. O'Hanlon , A. Oblakowska-Mucha , V. Obraztsov , S. Ogilvy , O. Okhrimenko , R. Oldeman , C. J. G. Onderwater , B. Osorio Rodrigues , J. M. Otalora Goicochea , A. Otto , P. Owen , A. Oyanguren , A. Palano , F. Palombo , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , L. L. Pappalardo , C. Pappenheimer , W. Parker , C. Parkes , G. Passaleva , G. D. Patel , M. Patel , C. Patrignani , A. Pearce , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , P. Perret , L. Pescatore , K. Petridis , A. Petrolini , M. Petruzzo , E. Picatoste Olloqui , B. Pietrzyk , T. Pilař , D. Pinci , A. Pistone , A. Piucci , S. Playfer , M. Plo Casasus , T. Poikela , F. Polci , A. 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Yushchenko , M. Zangoli , M. Zavertyaev , L. Zhang , Y. Zhang , A. Zhelezov , A. Zhokhov , L. Zhong , S. Zucchelli

Contributions to the muon anomalous magnetic moment are evaluated in the technicolor model with scalars and topcolor assisted technicolor model. In the technicolor model with scalars, the additional contributions come from the loops of…

High Energy Physics - Phenomenology · Physics 2009-11-07 Z. Xiong , J. M. Yang

The reported discrepancy of the muon abnormal magnetic moment $a_\mu^{}$ has impacts on the low energy phenomenology. In this paper we calculate the corrections to $a_\mu$ in the standard model extended by the TeV scale seesaw models. We…

High Energy Physics - Phenomenology · Physics 2008-06-06 Wei Chao

The increasing accuracy of current and planned experiments to measure the anomalous magnetic moment of the muon requires more precision and reliability of its theoretical calculation. For this purpose, we calculate the differential cross…

High Energy Physics - Phenomenology · Physics 2023-08-21 V. S. Fadin , R. N. Lee

We study meson loop corrections to the baryon magnetic moments starting from a QCD-based quark model derived earlier in a quenched approximation to QCD. The model reproduces the standard quark model with extra corrections for the binding of…

High Energy Physics - Phenomenology · Physics 2009-10-31 Phuoc Ha , Loyal Durand

Neutrino mass hierarchy can be measured in atmospheric neutrino experiments through the observation of earth matter effects. Magnetized iron calorimeters have been shown to be good in this regard due to their charge identification…

High Energy Physics - Phenomenology · Physics 2015-06-16 Anushree Ghosh , Sandhya Choubey

The MUSE experiment at the Paul Scherrer Institute is measuring elastic lepton-proton scattering cross sections in a four-momentum transfer range from $Q^2$ of approximately 0.002 to 0.08 GeV$^2$ using positively and negatively charged…

The radiative muon capture(RMC) on a proton is analyzed by means of heavy baryon chiral perturbation theory. The emitted photon energy spectrum is calculated and compared with the experimental data by taking the spin sum on the muonic atom…

High Energy Physics - Phenomenology · Physics 2009-10-30 Shung-ichi Ando , Dong-Pil Min

The impact of higher-order final-state photonic corrections on the precise determination of the W-boson mass at the Tevatron and LHC colliders is evaluated. The W-mass shift from a fit to the transverse mass distribution is found to be…

High Energy Physics - Phenomenology · Physics 2011-09-13 C. M. Carloni Calame , G. Montagna , O. Nicrosini , M. Treccani

The anomalous magnetic moments of both positive and negative muons are measured to the precision of 0.7 parts per million. Two values are in good agreement. The standard model calculations of muon g-2 are under further studies, especially…

High Energy Physics - Experiment · Physics 2007-05-23 H. Deng , for Muon g-2 Collaboration

The E821 experiment at Brookhaven National Laboratory is designed to measure the muon magnetic anomaly, a_mu, to an ultimate precision of 0.4 parts per million (ppm). Because theory can predict a_mu to 0.6 ppm, and ongoing efforts aim to…

High Energy Physics - Experiment · Physics 2017-08-23 David W. Hertzog

We present a measurement of the ratio of positive to negative muon fluxes from cosmic ray interactions in the atmosphere, using data collected by the CMS detector both at ground level and in the underground experimental cavern at the CERN…

High Energy Physics - Experiment · Physics 2012-08-27 The CMS Collaboration

Cosmic ray muons have been considered as a non-conventional radiation probe in various applications. To utilize cosmic ray muons in engineering applications, two important quantities, trajectory and momentum, must be known. The muon…

Instrumentation and Detectors · Physics 2022-01-04 Junghyun Bae , Stylianos Chatzidakis

The most recent high-precision determination of the hadronic leading order contribution to the muon magnetic dipole moment within the Standard Model of particle physics has revealed a five standard deviation discrepancy with the previous…

High Energy Physics - Phenomenology · Physics 2023-10-06 Noah Bray-Ali
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