English
Related papers

Related papers: Using the Fermilab Proton Source for a Muon to Ele…

200 papers

The Fermilab Proton-Improvement-Plan-II (PIP-II) is being implemented in order to support the precision neutrino oscillation measurements at the Deep Underground Neutrino Experiment, the U.S. flagship neutrino experiment. The PIP-II LINAC…

The Mu2e experiment at Fermilab proposes to search for the coherent neutrino-less conversion of muons to electrons in the presence of a nucleus. The experimental signature for an aluminum target is an isolated 105 MeV electron exiting the…

Accelerator Physics · Physics 2015-11-09 S. Boi , A. Dyshkant , D. Hedin , E. Johnson , E. Prebys , P. Rubinov

An energetic muon beam is an attractive key to unlock new physics beyond the Standard Model: the lepton flavor violation or the anomalous magnetic moment, and also is a competitive candidate for the expected neutrino factory. Lots of the…

Accelerator Physics · Physics 2024-06-19 Xiao-Nan Wang , Xiao-Fei Lan , Yong-Sheng Huang , Hao Zhang , Tong-Pu Yu

We report the results of a search for muon-neutrino disappearance by the Main Injector Neutrino Oscillation Search. The experiment uses two detectors separated by 734 km to observe a beam of neutrinos created by the Neutrinos at the Main…

High Energy Physics - Experiment · Physics 2019-08-13 Michael Kordosky , David Petyt

Knowledge of the neutrino flux produced by the Neutrinos at the Main Injector (NuMI) beamline is essential to the neutrino oscillation and neutrino interaction measurements of the MINERvA, MINOS+, NOvA and MicroBooNE experiments at Fermi…

Fermilab operates the world's most intense antiproton source. Recently proposed experiments can use those antiprotons either parasitically during Tevatron Collider running or after the Tevatron Collider finishes in about 2011. For example,…

High Energy Physics - Phenomenology · Physics 2010-08-02 Daniel M. Kaplan

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

I describe the new generation of muon-to-electron conversion experiments, COMET and Mu2e, being constructed to make use of new high power pulsed muon beams a J-PARC and Fermilab respectively. A brief overview of the physics explored by the…

Instrumentation and Detectors · Physics 2014-12-04 R. P. Litchfield

The Neutrinos at the Main Injector (NuMI) facility is a conventional horn-focused neutrino beam which produces muon neutrinos from a beam of mesons directed into a long evacuated decay volume. The relative alignment of the primary proton…

High energy and high beam power accelerators are extensively used for the neutrino physics research. At present, the leading operational facilities are the Fermilab Main Injector complex that delivers over 0.75 MW of 120 GeV protons on the…

Accelerator Physics · Physics 2019-06-19 Vladimir Shiltsev

Searches for dark-matter particles at the GeV mass scale has been receiving much attention in the last several years, partly motivated by the failure of direct and indirect searches of heavier candidates to produce a signal. The SpinQuest…

Instrumentation and Detectors · Physics 2019-10-17 Vassili Papavassiliou

Neutrinos from STORed Muons (nuSTORM; formerly VLENF) is a proposed experiment to use 3.8 GeV/c muon decay to produce a well-understood beam of electron and muon neutrinos that can be used for short baseline physics. A magnetized far…

High Energy Physics - Phenomenology · Physics 2012-06-08 C. D. Tunnell

A search for long-lived neutral particles (N^0's) with masses above 2.2 GeV/c^2 that decay into at least one muon has been performed using an instrumented decay channel at the NuTeV experiment at Fermilab. Data were examined for particles…

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

We explore the physics potential of the NuMI beamline with a detector located 10 km off-axis at a distant site (810 km). We study the sensitivity to $\sin^2 2 \theta_{13}$ and to the CP-violating parameter $\sin \delta$ as well as the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Olga Mena , Stephen Parke

The potentially realizable beam power at the Fermilab long-baseline neutrino program has motivated a reinvigorated design and optimization effort for a rapid-cycling synchrotron (RCS) intensity upgrade of the Fermilab proton complex. We…

Accelerator Physics · Physics 2020-01-17 Jeffrey Eldred

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

The ArgoNeuT collaboration presents measurements of inclusive muon neutrino and antineutrino charged current differential cross sections on argon in the Fermilab NuMI beam operating in the low energy antineutrino mode. The results are…

The NuMI Off-Axis v Appearance (NOvA) experiment is a long baseline neutrino oscillation experiment using a neutrino source created from the NuMI Beamline at Fermilab. The experiment will study the oscillations of muon neutrinos to electron…

Instrumentation and Detectors · Physics 2011-09-27 N. Raddatz

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 4 5 6 7 8 10 Next ›