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Permanent electric dipole moments (EDMs) are excellent probes of physics beyond the Standard Model, especially on new sources of CP violation. The muon EDM has recently attracted significant attention due to discrepancies in the magnetic…

The Muon Ionization Cooling Experiment (MICE) is a strategic R&D project intended to demonstrate the only practical solution to providing high brilliance beams necessary for a neutrino factory or muon collider. MICE is under development at…

Accelerator Physics · Physics 2013-08-01 U. Bravar , M. Bogomilov , Y. Karadzhov , D. Kolev , I. Russinov , R. Tsenov , L. Wang , F. Y. Xu , S. X. Zheng , R. Bertoni , M. Bonesini , R. Mazza , V. Palladino , G. Cecchet , A. de Bari , M. Capponi , A. Iaciofano , D. Orestano , F. Pastore , L. Tortora , S. Ishimoto , S. Suzuki , K. Yoshimura , Y. Mori , Y. Kuno , H. Sakamoto , A. Sato , T. Yano , M. Yoshida , F. Filthaut , M. Vretenar , S. Ramberger , A. Blondel , F. Cadoux , F. Masciocchi , J. S. Graulich , V. Verguilov , H. Wisting , C. Petitjean , R. Seviour , M. Ellis , P. Kyberd , M. Littlefield , J. J. Nebrensky , D. Forrest , F. J. P. Soler , K. Walaron , P. Cooke , R. Gamet , A. Alecou , M. Apollonio , G. Barber , A. Dobbs , P. Dornan , A. Fish , R. Hare , A. Jamdagni , V. Kasey , M. Khaleeq , K. Long , J. Pasternak , H. Sakamoto , T. Sashalmi , V. Blackmore , J. Cobb , W. Lau , M. Rayner , C. D. Tunnell , H. Witte , S. Yang , J. Alexander , G. Charnley , S. Griffiths , B. Martlew , A. Moss , I. Mullacrane , A. Oats , S. York , R. Apsimon , R. J. Alexander , P. Barclay , D. E. Baynham , T. W. Bradshaw , M. Courthold , R. Edgecock T. Hayler , M. Hills , T. Jones , N. McCubbin , W. J. Murray , C. Nelson , A. Nicholls , P. R. Norton , C. Prior , J. H. Rochford , C. Rogers , W. Spensley , K. Tilley , C. N. Booth , P. Hodgson , R. Nicholson , E. Overton , M. Robinson , P. Smith , D. Adey , J. Back , S. Boyd , P. Harrison , J. Norem , A. D. Bross , S. Geer , A. Moretti , D. Neuffer , M. Popovic , Z. Qian , R. Raja , R. Stefanski , M. A. C. Cummings , T. J. Roberts , A. DeMello , M. A. Green , D. Li , A. M. Sessler , S. Virostek , M. S. Zisman , B. Freemire , P. Hanlet , D. Huang , G. Kafka , D. M. Kaplan , P. Snopok , Y. Torun , Y. Onel , D. Cline , K. Lee , Y. Fukui , X. Yang , R. A. Rimmer , L. M. Cremaldi , T. L. Hart , D. J. Summers , L. Coney , R. Fletcher , G. G. Hanson , C. Heidt , J. Gallardo , S. Kahn , H. Kirk , R. B. Palmer

We propose here a proposal to connect neutrino and energy frontiers, by exploiting collimated muon beams for neutrino oscillations, which generate symmetric neutrino and antineutrino sources: $\mu^+\rightarrow e^+\,\bar{\nu}_{\mu}\,…

High Energy Physics - Phenomenology · Physics 2023-10-31 Alim Ruzi , Tianyi Yang , Dawei Fu , Sitian Qian , Leyun Gao , Qiang Li

We report results from the MuLan measurement of the positive muon lifetime. The experiment was conducted at the Paul Scherrer Institute using a time-structured surface muon beam and a segmented plastic scintillator array. Two different…

High Energy Physics - Experiment · Physics 2013-01-04 T. P. Gorringe

The muonium atom is the purely leptonic bound state of a positive muon and an electron. It has a lifetime of 2.2 $\mu$s. The absence of any known internal structure provides for precision experiments to test fundamental physics theories and…

High Energy Physics - Experiment · Physics 2016-08-03 Klaus P. Jungmann

Recently the atmospheric muon spectra at high energies were reconstructed for two ranges of zenith angles, basing on the events collected with the IceCube detector. These measurements reach high energies at which the contribution to…

High Energy Physics - Phenomenology · Physics 2019-07-02 A. A. Kochanov , A. D. Morozova , T. S. Sinegovskaya , S. I. Sinegovsky

The study of novel quantum materials relies on muon-spin rotation, relaxation, or resonance (\mSR) measurements. Yet, a fundamental limitation persists: many of these materials can only be synthesized in extremely small quantities, often at…

We demonstrate efficient transverse compression of a 12.5 MeV/c muon beam stopped in a helium gas target featuring a vertical density gradient and crossed electric and magnetic fields. The muon stop distribution extending vertically over 14…

Muon colliders offer special opportunities to discover and study new physics. With the high intensity source of muons at the front end, orders of magnitude improvements would be realized in searches for rare muon processes, in deep…

High Energy Physics - Phenomenology · Physics 2009-10-31 V. Barger

A neutron source is proposed. It is based on a proton accelerator with the energy Ep = 1.2 GeV, current Ip = 0.7A, pulse duration T = 3 mcsec, repetition rate F = 60 Hz, and accelerator length L = 30 m. Protons are accelerated by the field…

Accelerator Physics · Physics 2009-08-05 S. N. Dolya , K. A. Reshetnikova

The low-energy muon facility at PSI provides nearly fully polarized positive muons with tunable energies in the keV range to carry out muon spin rotation (LE-muSR) experiments with nanometer depth resolution on thin films, heterostructures,…

Accelerator Physics · Physics 2017-02-08 Ran Xiao , Elvezio Morenzoni , Zaher Salman , Bangjiao Ye , Thomas Prokscha

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

We have measured the muon flux at the underground Gran Sasso National Laboratory (3800 m w.e.) to be (3.41 \pm 0.01) \times 10-4m-2s-1 using four years of Borexino data. A modulation of this signal is observed with a period of (366\pm3)…

The High Intensity Proton Accelerator (HIPA) cyclotron at the Paul Scherrer Institut (PSI) delivers 590 MeV CW proton beam with a maximum power of 1.42 MW. After extraction, the beam is transferred in a 120 m long channel towards two target…

Accelerator Physics · Physics 2022-11-23 M. Haj Tahar , D. Kiselev , A. Knecht , D. Laube , D. Reggiani , J. Snuverink

The mean life of the positive muon has been measured to a precision of 11 ppm using a low-energy, pulsed muon beam stopped in a ferromagnetic target, which was surrounded by a scintillator detector array. The result, tau_mu = 2.197013(24)…

A high-statistics determination of the differential cross section of elastic muon-electron scattering as a function of the transferred four-momentum squared, $d \sigma_{el}(\mu e \to \mu e)/dq^2$, has been argued to provide an effective…

Instrumentation and Detectors · Physics 2020-02-25 Tommaso Dorigo

The search for feebly-interacting new-physics particles in the MeV-GeV mass range often involves high-intensity beams dumped into thick heavy targets. The challenge of evaluating the expected backgrounds for these searches from first…

High Energy Physics - Experiment · Physics 2021-09-15 Stefan Ghinescu , Babette Döbrich , Elisa Minucci , Tommaso Spadaro

Muon energy measurement represents an important issue for any experiment addressing neutrino induced upgoing muon studies. Since the neutrino oscillation probability depends on the neutrino energy, a measurement of the muon energy adds an…

Instrumentation and Detectors · Physics 2012-08-27 The MACRO Collaboration

We introduce a new search strategy for visibly decaying muonphilic particles using a proton beam spectrometer modeled after the SpinQuest experiment at Fermilab. In this setup, a ${\sim}$100 GeV primary proton beam impinges on a thick fixed…

High Energy Physics - Phenomenology · Physics 2023-07-12 Diana Forbes , Christian Herwig , Yonatan Kahn , Gordan Krnjaic , Cristina Mantilla Suarez , Nhan Tran , Andrew Whitbeck

The Muon $(g-2)$ experiment, E821, at the Brookhaven AGS has the goal to measure the muon anomalous magnetic moment to a relative accuracy of $\pm 3.5 \times 10^{-7}$. A superferric 14 m diameter storage ring has been constructed and an…

High Energy Physics - Experiment · Physics 2007-05-23 B. Lee Roberts