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Muon ionization cooling provides the only practical solution to prepare high-brilliance beams necessary for a neutrino factory or muon collider. The Muon Ionization Cooling Experiment (MICE), under development at the Rutherford Appleton…

Accelerator Physics · Physics 2008-10-11 Terrence L. Hart , Daniel M. Kaplan

The intensities and profiles of the muon beam behind the beam dump of the Fermilab test beam area when the facility is running in the "pion" beam mode are measured and summarized in this note. This muon beam with momenta in the range 10 -…

Accelerator Physics · Physics 2016-08-12 Dmitri Denisov , Valery Evdokimov , Strahinja Lukić , Predrag Ujić

In this paper we stress the idea that new, more precise neutrino cross-sections measurements at low energies will be necessary to improve the results of future big neutrino detectors, which will be dominated by the contribution of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Campanelli , S. Navas-Concha , A. Rubbia

The $\mu$E4-LEM beamline at Paul Scherrer Institute (PSI, Switzerland) is a special muon beamline combining the hyprid type surface muon beamline $\mu$E4 with the low energy muon facility (LEM) and delivers ${\mu}^{+}$ with tunable energy…

Accelerator Physics · Physics 2022-03-28 Lu-Ping Zhou , Xiao-Jie Ni , Zaher Salman , Andreas Suter , Jing-Yu Tang , Vjeran Vrankovic , Thomas Prokscha

A novel single-particle technique to measure emittance has been developed and used to characterise seventeen different muon beams for the Muon Ionisation Cooling Experiment (MICE). The muon beams, whose mean momenta vary from 171 to 281…

Accelerator Physics · Physics 2013-10-14 The MICE Collaboration , D. Adams , D. Adey , A. Alekou , M. Apollonio , R. Asfandiyarov , J. Back , G. Barber , P. Barclay , A. de Bari , R. Bayes , V. Bayliss , R. Bertoni , V. J. Blackmore , A. Blondel , S. Blot , M. Bogomilov , M. Bonesini , C. N. Booth , D. Bowring , S. Boyd , T. W. Bradshaw , U. Bravar , A. D. Bross , M. Capponi , T. Carlisle , G. Cecchet , G. Charnley , J. H. Cobb , D. Colling , N. Collomb , L. Coney , P. Cooke , M. Courthold , L. M. Cremaldi , A. DeMello , A. Dick , A. Dobbs , P. Dornan , S. Fayer , F. Filthaut , A. Fish , T. Fitzpatrick , R. Fletcher , D. Forrest , V. Francis , B. Freemire , L. Fry , A. Gallagher , R. Gamet , S. Gourlay , A. Grant , J. S. Graulich , S. Griffiths , P. Hanlet , O. M. Hansen , G. G. Hanson , P. Harrison , T. L. Hart , T. Hartnett , T. Hayler , C. Heidt , M. Hills , P. Hodgson , A. Iaciofano , S. Ishimoto , G. Kafka , D. M. Kaplan , Y. Karadzhov , Y. K. Kim , D. Kolev , Y. Kuno , P. Kyberd , W. Lau , J. Leaver , M. Leonova , D. Li , A. Lintern , M. Littlefield , K. Long , G. Lucchini , T. Luo , C. Macwaters , B. Martlew , J. Martyniak , A. Moretti , A. Moss , A. Muir , I. Mullacrane , J. J. Nebrensky , D. Neuffer , A. Nichols , R. Nicholson , J. C. Nugent , Y. Onel , D. Orestano , E. Overton , P. Owens , V. Palladino , J. Pasternak , F. Pastore , C. Pidcott , M. Popovic , R. Preece , S. Prestemon , D. Rajaram , S. Ramberger , M. A. Rayner , S. Ricciardi , A. Richards , T. J. Roberts , M. Robinson , C. Rogers , K. Ronald , P. Rubinov , R. Rucinski , I. Rusinov , H. Sakamoto , D. A. Sanders , E. Santos , T. Savidge , P. J. Smith , P. Snopok , F. J. P. Soler , T. Stanley , D. J. Summers , M. Takahashi , J. Tarrant , I. Taylor , L. Tortora , Y. Torun , R. Tsenov , C. D. Tunnell , G. Vankova , V. Verguilov , S. Virostek , M. Vretenar , K. Walaron , S. Watson , C. White , C. G. Whyte , A. Wilson , H. Wisting , M. Zisman

The international Muon Ionization Cooling Experiment (MICE) will perform a systematic investigation of ionization cooling with muon beams of momentum between 140 and 240\,MeV/c at the Rutherford Appleton Laboratory ISIS facility. The…

Instrumentation and Detectors · Physics 2016-03-03 D. Adams , A. Alekou , M. Apollonio , R. Asfandiyarov , G. Barber , P. Barclay , A. de Bari , R. Bayes , V. Bayliss , R. Bertoni , V. J. Blackmore , A. Blondel , S. Blot , M. Bogomilov , M. Bonesini , C. N. Booth , D. Bowring , S. Boyd , T. W. Bradshaw , U. Bravar , A. D. Bross , M. Capponi , T. Carlisle , G. Cecchet , C. Charnley , F. Chignoli , D. Cline , J. H. Cobb , G. Colling , N. Collomb , L. Coney , P. Cooke , M. Courthold , L. M. Cremaldi , A. DeMello , A. Dick , A. Dobbs , P. Dornan , M. Drews , F. Drielsma , F. Filthaut , T. Fitzpatrick , P. Franchini , V. Francis , L. Fry , A. Gallagher , R. Gamet , R. Gardener , S. Gourlay , A. Grant , J. R. Greis , S. Griffiths , P. Hanlet , O. M. Hansen , G. G. Hanson , T. L. Hart , T. Hartnett , T. Hayler , C. Heidt , M. Hills , P. Hodgson , C. Hunt , A. Iaciofano , S. Ishimoto , G. Kafka , D. M. Kaplan , Y. Karadzhov , Y. K. Kim , Y. Kuno , P. Kyberd , J-B Lagrange , J. Langlands , W. Lau , M. Leonova , D. Li , A. Lintern , M. Littlefield , K. Long , T. Luo , C. Macwaters , B. Martlew , J. Martyniak , R. Mazza , S. Middleton , A. Moretti , A. Moss , A. Muir , I. Mullacrane , J. J. Nebrensky , D. Neuffer , A. Nichols , R. Nicholson , J. C. Nugent , A. Oates , Y. Onel , D. Orestano , E. Overton , P. Owens , V. Palladino , J. Pasternak , F. Pastore , C. Pidcott , M. Popovic , R. Preece , S. Prestemon , D. Rajaram , S. Ramberger , M. A. Rayner , S. Ricciardi , T. J. Roberts , M. Robinson , C. Rogers , K. Ronald , P. Rubinov , P. Rucinski , H. Sakamato , D. A. Sanders , E. Santos , T. Savidge , P. J. Smith , P. Snopok , F. J. P. Soler , D. Speirs , T. Stanley , G. Stokes , D. J. Summers , J. Tarrant , I. Taylor , L. Tortora , Y. Torun , R. Tsenov , C. D. Tunnell , M. A. Uchida , G. Vankova-Kirilova , S. Virostek , M. Vretenar , P. Warburton , S. Watson , C. White , C. G. Whyte , A. Wilson , M. Winter , X. Yang , A. Young , M. Zisman

Ordinary muon capture provides a benchmark for the nuclear physics models of neutrinoless double beta decay under comparable momentum transfer conditions. The total capture strength defines the lifetime of the muonic atom. The muon lifetime…

High-intensity high-energy neutrino beams could be produced by exploiting a very intense future muon source, and allowing the muons to decay in a storage ring containing a long straight section. Taking the parameters of muon source designs…

High Energy Physics - Phenomenology · Physics 2014-11-17 S. Geer

The power supply studies for the four-horn system for the CERN to Fr\'ejus neutrino Super Beam oscillation experiment are discussed here. The power supply is being studied to meet the physics potential and the mega-watt (MW) power…

Accelerator Physics · Physics 2014-07-01 E Baussan , E Bouquerel , M Dracos , G Gaudiot , F Osswald , P Poussot , N Vassilopoulos , J Wurtz , V Zeter

A 4600 Hz fast ramping synchrotron is explored as an economical way of accelerating muons from 4 to 20 GeV/c for a neutrino factory. Eddy current losses are minimized by the low machine duty cycle plus thin grain oriented silicon steel…

High Energy Physics - Experiment · Physics 2008-11-26 D. J. Summers , J. S. Berg , A. A. Garren , R. B. Palmer

Muon ionization cooling provides the only practical solution for preparing high brightness beams necessary for a neutrino factory or muon collider. The Muon Ionization Cooling Experiment (MICE) is under development at the Rutherford…

Instrumentation and Detectors · Physics 2009-10-20 L. Coney

The Muon Scattering Experiment at the Paul Scherrer Institut uses a mixed beam of electrons, muons, and pions, necessitating precise timing to identify the beam particles and reactions they cause. We describe the design and performance of…

The muLan experiment at the Paul Scherrer Institute will measure the lifetime of the positive muon with a precision of 1 ppm, giving a value for the Fermi coupling constant G_F at the level of 0.5 ppm. Meanwhile, by measuring the observed…

Nuclear Experiment · Physics 2020-05-20 F. E. Gray

An "ultimate" high intensity proton source for neutrino factories and/or muon colliders was projected to be a ~4 MW multi-GeV proton source providing short, intense proton pulses at ~15 Hz. The JPARC ~1 MW accelerators provide beam at…

Accelerator Physics · Physics 2017-04-27 D. Neuffer

We present the detection of directional muon beams produced using a PW laser at the Lawrence Berkeley National Laboratory. The muon source is a multi-GeV electron beam generated in a 30 cm laser plasma accelerator interacting with a high-Z…

The experimental evidence that \theta_{13} is large opens new opportunities to identify the neutrino mass spectrum. We outline a possibility to investigate this issue by means of conventional technology. The ideal setup turns out to be long…

High Energy Physics - Phenomenology · Physics 2013-06-04 Carolina Lujan-Peschard , Giulia Pagliaroli , Francesco Vissani

Muons, which play a crucial role in both fundamental and applied physics, have traditionally been generated through proton accelerators or from cosmic rays. With the advent of ultra-short high-intensity lasers capable of accelerating…

Using a sample of 38.5 million underground muons collected by the MACRO detector we have performed an all-sky search for pointlike sources producing excesses of muons above the expected background. The d.c. muon flux upper limit at the…

High Energy Physics - Experiment · Physics 2019-08-14 C. Satriano
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