English
Related papers

Related papers: Workshop on a future muon program at FNAL

200 papers

The Muon Campus at Fermilab provides world class accelerator infrastructure supporting the next generation intensity frontier experiments. The anti-proton source from the Tevatron era was converted to the present day Muon Campus at the end…

Accelerator Physics · Physics 2022-08-08 S. Ganguly

The workshop titled "US Muon Workshop 2021: A road map for a future Muon Facility" was held virtually on February 1-2, 2021. The workshop aimed to bring together world experts in muon spectroscopy ($\mu$SR) and other techniques along with…

Instrumentation and Detectors · Physics 2022-08-08 Despina Louca , Gregory J. MacDougall , Travis J. Williams

The upcoming muon (g-2) experiment at Fermilab will measure the anomalous magnetic moment of the muon to a relative precision of 140 ppb, 4 times better than the previous experiment at BNL. The new experiment is motivated by the persistent…

Instrumentation and Detectors · Physics 2015-04-07 J. Kaspar

The use of existing Fermilab facilities to provide beams for two muon experiments -- the Muon to Electron Conversion Experiment (Mu2e) and the New g-2 Experiment -- is under consideration. Plans are being pursued to perform these…

Accelerator Physics · Physics 2009-10-20 M. J. Syphers

The Muon g-2 experiment at Fermilab, with the aim to measure the muon anomalous magnetic moment to an unprecedented level of 140~ppb, has started beam and detector commissioning in Summer 2017. To deal with incoming data projected to be…

Instrumentation and Detectors · Physics 2019-08-14 Kim Siang Khaw

A staged approach towards muon based facilities for Intensity and Energy Frontier science, building upon existing and proposed facilities at Fermilab, is presented. At each stage, a facility exploring new physics also provides an R&D…

I report on the progress of two new muon anomalous magnetic moment experiments, which are in advanced design and construction phases. The goal of Fermilab E989 is to reduce the experimental uncertainty of $a_\mu$ from Brookhaven E821 by a…

High Energy Physics - Experiment · Physics 2016-06-22 David W. Hertzog

The muon anomalous magnetic moment, $a_\mu = (g-2)/2$, is a low-energy observable which can be both measured and computed with very high precision, making it an excellent test of the Standard Model (SM) and a sensitive probe of new physics.…

High Energy Physics - Experiment · Physics 2022-07-20 Paolo Girotti

A precision measurement of the muon anomalous magnetic moment, $a_{\mu} = (g-2)/2$, was previously performed at BNL with a result of 2.2 - 2.7 standard deviations above the Standard Model (SM) theoretical calculations. The same experimental…

Accelerator Physics · Physics 2013-01-30 C. Yoshikawa , A. Leveling , N. V. Mokhov , J. Morgan , D. Neuffer , S. Striganov

Charged lepton flavor violation (CLFV) is expected in a diverse set of new physics scenarios. The current generation of experiments probe CLFV in the muon sector in three complementary channels: $\mu^-N \rightarrow e^- N$ (Mu2e, COMET),…

High Energy Physics - Experiment · Physics 2025-01-28 Sophie Middleton

The Muon (g-2) Experiment, E989 at Fermilab, will measure the muon anomalous magnetic moment a factor-of-four more precisely than was done in E821 at the Brookhaven National Laboratory AGS. The E821 result appears to be greater than the…

Instrumentation and Detectors · Physics 2018-05-15 J. Grange , V. Guarino , P. Winter , K. Wood , H. Zhao , R. M. Carey , D. Gastler , E. Hazen , N. Kinnaird , J. P. Miller , J. Mott , B. L. Roberts , J. Benante , J. Crnkovic , W. M. Morse , H. Sayed , V. Tishchenko , V. P. Druzhinin , B. I. Khazin , I. A. Koop , I. Logashenko , Y. M. Shatunov , E. Solodov , M. Korostelev , D. Newton , A. Wolski , A. Chapelain , R. Bjorkquist , N. Eggert , A. Frankenthal , L. Gibbons , S. Kim , A. Mikhailichenko , Y. Orlov , D. Rubin , D. Sweigart , D. Allspach , G. Annala , E. Barzi , K. Bourland , G. Brown , B. C. K. Casey , S. Chappa , M. E. Convery , B. Drendel , H. Friedsam , T. Gadfort , K. Hardin , S. Hawke , S. Hayes , W. Jaskierny , C. Johnstone , J. Johnstone , V. Kashikhin , C. Kendziora , B. Kiburg , A. Klebaner , I. Kourbanis , J. Kyle , N. Larson , A. Leveling , A. L. Lyon , D. Markley , D. McArthur , K. W. Merritt , N. Mokhov , J. P. Morgan , H. Nguyen , J-F. Ostiguy , A. Para , C. C. Polly M. Popovic , E. Ramberg , M. Rominsky , D. Schoo , R. Schultz , D. Still , A. K. Soha , S. Strigonov , G. Tassotto , D. Turrioni , E. Villegas , E. Voirin , G. Velev , L. Welty-Rieger , D. Wolff , C. Worel , J-Y. Wu , R. Zifko , K. Jungmann , C. J. G. Onderwater , P. T. Debevec , S. Ganguly , M. Kasten , S. Leo , K. Pitts , C. Schlesier , M. Gaisser , S. Haciomeroglu , Y-I. Kim , S. Lee , M-J Lee , Y. K. Semertzidis , K. Giovanetti , V. A. Baranov , V. N. Duginov , N. V. Khomutov , V. A. Krylov , N. A. Kuchinskiy , V. P. Volnykh , C. Crawford , R. Fatemi , W. P. Gohn , T. P. Gorringe , W. Korsch , B. Plaster , A. Anastasi , D. Babusci , S. Dabagov , C. Ferrari , A. Fioretti , C. Gabbanini , D. Hampai , A. Palladino , G. Venanzoni , T. Bowcock , J. Carroll , B. King , S. Maxfield , K. McCormick , J. Price , D. Sim , A. Smith , T. Teubner , W. Turner , M. Whitley , M. Wormald , R. Chislett , S. Kilani , M. Lancaster , E. Motuk , T. Stuttard , M. Warren , D. Flay , D. Kawall , Z. Meadows , T. Chupp , R. Raymond , A. Tewlsey-Booth , M. J. Syphers , D. Tarazona , S. Catalonotti , R. Di Stefano , M. Iacovacci , S. Mastroianni , S. Chattopadhyay , M. Eads , M. Fortner , D. Hedin , N. Pohlman , A. de Gouvea , H. Schellman , L. Welty-Rieger , F. Azfar , S. Henry , G. D. Alkhazov , V. L. Golovtsov , P. V. Neustroev , L. N. Uvarov , A. A. Vasilyev , A. A. Vorobyov , M. B. Zhalov , L. Cerrito , F. Gray , G. Di Sciascio , D. Moricciani , C. Fu , X. Ji , L. Li , H. Yang , D. Stöckinger , G. Cantatore , D. Cauz , M. Karuza , G. Pauletta , L. Santi , S. Baeßler , M. Bychkov , E. Frlez , D. Pocanic , L. P. Alonzi , M. Fertl , A. Fienberg , N. Froemming , A. Garcia , D. W. Hertzog J. Kaspar , P. Kammel , R. Osofsky , M. Smith , E. Swanson , T. van Wechel , K. Lynch

The precise measurement of the muon anomalous magnetic moment $a_\mathrm{\mu}$ has stimulated much theoretical and experimental efforts over more than six decades. The last experiment at Brookhaven National Laboratory, Upton, NY, USA…

Instrumentation and Detectors · Physics 2016-10-25 Martin Fertl

The E989 Muon $g-2$ Experiment at Fermilab aims to measure the muon magnetic anomaly, $a_\mu$, to an unprecedented precision of 140 parts per billion (ppb), representing a four-fold improvement over the current best measurement, achieved at…

High Energy Physics - Experiment · Physics 2019-05-15 A. T. Fienberg

Muon-based facilities offer unique potential to provide capabilities at both the Intensity Frontier with Neutrino Factories and the Energy Frontier with Muon Colliders. They rely on a novel technology with challenging parameters, for which…

The Muon $g\textrm{-}2$ Experiment (E989) at Fermilab has a goal of measuring the muon anomaly ($a_\mu$) with unprecedented precision using positive muons. This measurement is motivated by the difference between the previous Brookhaven…

Accelerator Physics · Physics 2020-09-25 Eremey Valetov

A multi-TeV muon collider offers a spectacular opportunity in the direct exploration of the energy frontier. Offering a combination of unprecedented energy collisions in a comparatively clean leptonic environment, a high energy muon…

High Energy Physics - Experiment · Physics 2023-08-10 K. M. Black , S. Jindariani , D. Li , F. Maltoni , P. Meade , D. Stratakis , D. Acosta , R. Agarwal , K. Agashe , C. Aime , D. Ally , A. Apresyan , A. Apyan , P. Asadi , D. Athanasakos , Y. Bao , E. Barzi , N. Bartosik , L. A. T. Bauerdick , J. Beacham , S. Belomestnykh , J. S. Berg , J. Berryhill , A. Bertolin , P. C. Bhat , M. E. Biagini , K. Bloom , T. Bose , A. Bross , E. Brost , N. Bruhwiler , L. Buonincontri , D. Buttazzo , V. Candelise , A. Canepa , L. Carpenter , M. Casarsa , F. Celiberto , C. Cesarotti , G. Chachamis , Z. Chacko , P. Chang , S. V. Chekanov , T. Y. Chen , M. Chiesa , T. Cohen , M. Costa , N. Craig , A. Crivellin , C. Curatolo , D. Curtin , G. Da Molin , S. Dasu , A. de Gouvea , D. Denisov , R. Dermisek , K. F. Di Petrillo , T. Dorigo , J. M. Duarte , V. D. Elvira , R. Essig , P. Everaerts , J. Fan , M. Felcini , G. Fiore , D. Fiorina , M. Forslund , R. Franceschini , M. V. Garzelli , C. E. Gerber , L. Giambastiani , D. Giove , S. Guiducci , T. Han , K. Hermanek , C. Herwig , J. Hirschauer , T. R. Holmes , S. Homiller , L. A. Horyn , A. Ivanov , B. Jayatilaka , H. Jia , C. K. Jung , Y. Kahn , D. M. Kaplan , M. Kaur , M. Kawale , P. Koppenburg , G. Krintiras , K. Krizka , B. Kuchma , L. Lee , L. Li , P. Li , Q. Li , W. Li , R. Lipton , Z. Liu , S. Lomte , Q. Lu , D. Lucchesi , T. Luo , K. Lyu , Y. Ma , P. A. N. Machado , C. Madrid , D. J. Mahon , A. Mazzacane , N. McGinnis , C. McLean , B. Mele , F. Meloni , S. C. Middleton , R. K. Mishra , N. Mokhov , A. Montella , M. Morandin , S. Nagaitsev , F. Nardi , M. S. Neubauer , D. V. Neuffer , H. Newman , R. Ogaz , I. Ojalvo , I. Oksuzian , T. Orimoto , B. Ozek , K. Pachal , S. Pagan Griso , P. Panci , V. Papadimitriou , N. Pastrone , K. Pedro , F. Pellemoine , A. Perloff , D. Pinna , F. Piccinini , Marc-Andre Pleier , S. Posen , K. Potamianos , S. Rappoccio , M. Reece , L. Reina , A. Reinsvold Hall , C. Riccardi , L. Ristori , T. Robens , R. Ruiz , P. Sala , D. Schulte , L. Sestini , V. Shiltsev , P. Snopok , G. Stark , J. Stupak , S . Su , R. Sundrum , M. Swiatlowski , M. J. Syphers , A. Taffard , W. Thompson , Y. Torun , C. G. Tully , I. Vai , M. Valente , U. van Rienen , R. van Weelderen , G. Velev , N. Venkatasubramanian , L. Vittorio , C. Vuosalo , X. Wang , H. Weber , R. Wu , Y. Wu , A. Wulzer , K. Xie , S. Xie , R. Yohay , K. Yonehara , F. Yu , A. V. Zlobin , D. Zuliani , J. Zurita

Fermilab is dedicated to hosting world-class experiments in search of new physics that will operate in the coming years. The Muon g-2 Experiment is one such experiment that will determine with unprecedented precision the muon anomalous…

The Fermilab Muon Campus will host the Muon g-2 experiment - a world class experiment dedicated to the search for signals of new physics. Strict demands are placed on beam diagnostics in order to ensure delivery of high quality beams to the…

Accelerator Physics · Physics 2017-09-19 D. Stratakis , B. Drendel , M. J. Syphers

The new g-2 experiment at Fermilab aims to measure the muon anomalous magnetic moment by a fourfold improvement in precision compared to the BNL experiment. Achieving this goal requires the delivery of highly polarized 3.094 GeV/c muons…

The upcoming Fermilab E989 experiment will measure the muon anomalous magnetic moment $a_{\mu}$ . This measurement is motivated by the previous measurement performed in 2001 by the BNL E821 experiment that reported a 3-4 standard deviation…

Instrumentation and Detectors · Physics 2017-04-05 Antoine Chapelain
‹ Prev 1 2 3 10 Next ›