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Related papers: Emittance Measurement in MICE

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The Muon Ionization Cooling Experiment (MICE) has measured the evolution of emittance due to ionization energy loss. Muons were focused onto an absorber using a large aperture solenoid. Lithium-hydride and liquid hydrogen- absorbers have…

Accelerator Physics · Physics 2018-06-13 Victoria Blackmore

Muon beams of low emittance provide the basis for the intense, well characterised neutrino beams of a neutrino factory and for multi-TeV lepton-antilepton collisions at a muon collider. The international Muon Ionization Cooling Experiment…

Accelerator Physics · Physics 2018-05-21 Paolo Franchini

The Muon Ionization Cooling Experiment (MICE) has been built at the STFC Rutherford Appleton Laboratory to demonstrate the principle of muon beam phase-space reduction via ionization cooling. Muon beam cooling will be required at a future…

Muon accelerators offer an attractive option for a range of future particle physics experiments. They can enable high energy (TeV+) high energy lepton colliders whilst mitigating the difficulty of synchrotron losses, and can provide intense…

The international Muon Ionization Cooling Experiment (MICE) aims to demonstrate muon beam ionization cooling for the first time and constitutes a key part of the R&D towards a future neutrino factory or muon collider. Beam cooling reduces…

Accelerator Physics · Physics 2019-08-15 Tanaz Angelina Mohayai , Pavel Snopok , David Neuffer , Chris Rogers

Muon storage rings have been proposed for use as sources of intense high-energy neutrino beams and as the basis for muon colliders. Phase-space compression (cooling) of the muon beam prior to acceleration and storage is needed to optimise…

High Energy Physics - Experiment · Physics 2008-11-26 P. Drumm

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 Muon Ionization Cooling Experiment (MICE) will perform a detailed study of ionization cooling to evaluate the feasibility of the technique. To carry out this program, MICE requires an efficient particle-identification (PID) system to…

Instrumentation and Detectors · Physics 2016-01-20 D. Adams , A. Alekou , M. Apollonio , R. Asfandiyarov , G. Barber , P. Barclay , A. de Bari , R. Bayes , V. Bayliss , P. Bene , 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 , F. Cadoux , 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 , S. Debieux , A. DeMello , A. Dick , A. Dobbs , P. Dornan , F. Drielsma , F. Filthaut , T. Fitzpatrick , P. Franchini , V. Francis , L. Fry , A. Gallagher , R. Gamet , R. Gardener , S. Gourlay , A. Grant , J. S. Graulich , J. 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 , C. Husi , 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 , F. Masciocchi , R. Mazza , S. Middleton , A. Moretti , A. Moss , A. Muir , I. Mullacrane , J. J. Nebrensky , D. Neuffer , A. Nichols , R. Nicholson , L. Nicola , E. Noah Messomo , 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 , K. Rothenfusser , P. Rubinov , P. Rucinski , H. Sakamato , D. A. Sanders , R. Sandstrom , 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 , H. Wisting , X. Yang , A. Young , M. Zisman

The International Muon Ionization Cooling Experiment (MICE) is devoted to a study of a muon cooling channel capable of giving the desired performance for a Neutrino Factory. One of the goals is achieving an absolute accuracy of measurements…

Accelerator Physics · Physics 2007-05-23 D. Errede , I. Rakhno

Accelerated muon beams have been considered for next-generation studies of high-energy lepton-antilepton collisions and neutrino oscillations. However, high-brightness muon beams have not yet been produced. The main challenge for muon…

Accelerator Physics · Physics 2023-10-16 The MICE Collaboration , M. Bogomilov , R. Tsenov , G. Vankova-Kirilova , Y. P. Song , J. Y. Tang , Z. H. Li , R. Bertoni , M. Bonesini , F. Chignoli , R. Mazza , A. de Bari , D. Orestano , L. Tortora , Y. Kuno , H. Sakamoto , A. Sato , S. Ishimoto , M. Chung , C. K. Sung , F. Filthaut , M. Fedorov , D. Jokovic , D. Maletic , M. Savic , N. Jovancevic , J. Nikolov , M. Vretenar , S. Ramberger , R. Asfandiyarov , A. Blondel , F. Drielsma , Y. Karadzhov , S. Boyd , J. R. Greis , T. Lord , C. Pidcott , I. Taylor , G. Charnley , N. Collomb , K. Dumbell , A. Gallagher , A. Grant , S. Griffiths , T. Hartnett , B. Martlew , A. Moss , A. Muir , I. Mullacrane , A. Oates , P. Owens , G. Stokes , P. Warburton , C. White , D. Adams , V. Bayliss , J. Boehm , T. W. Bradshaw , C. Brown , M. Courthold , J. Govans , T. Hayler , M. Hills , J. B. Lagrange , C. Macwaters , A. Nichols , R. Preece , S. Ricciardi , C. Rogers , T. Stanley , J. Tarrant , M. Tucker , S. Watson , A. Wilson , R. Bayes , J. C. Nugent , F. J. P. Soler , G. T. Chatzitheodoridis , A. J. Dick , K. Ronald , C. G. Whyte , A. R. Young , R. Gamet , P. Cooke , V. J. Blackmore , D. Colling , A. Dobbs , P. Dornan , P. Franchini , C. Hunt , P. B. Jurj , A. Kurup , K. Long , J. Martyniak , S. Middleton , J. Pasternak , M. A. Uchida , J. H. Cobb , C. N. Booth , P. Hodgson , J. Langlands , E. Overton , V. Pec , P. J. Smith , S. Wilbur , M. Ellis , R. B. S. Gardener , P. Kyberd , J. J. Nebrensky , A. DeMello , S. Gourlay , A. Lambert , D. Li , T. Luo , S. Prestemon , S. Virostek , M. Palmer , H. Witte , D. Adey , A. D. Bross , D. Bowring , A. Liu , D. Neuffer , M. Popovic , P. Rubinov , B. Freemire , P. Hanlet , D. M. Kaplan , T. A. Mohayai , D. Rajaram , P. Snopok , Y. Torun , L. M. Cremaldi , D. A. Sanders , L. R. Coney , G. G. Hanson , C. Heidt

The goal of the international Muon Ionization Cooling Experiment (MICE) is to demonstrate muon beam ionization cooling for the first time. It constitutes a key part of the R&D towards a future neutrino factory or muon collider. The intended…

Accelerator Physics · Physics 2018-06-06 Tanaz Angelina Mohayai , Pavel Snopok , David Neuffer

Muon colliders and neutrino factories are attractive options for future facilities aimed at achieving the highest lepton-antilepton collision energies and precision measurements of parameters of the Higgs boson and the neutrino mixing…

Accelerator Physics · Physics 2019-10-23 Daniel M. Kaplan

The Electron-Muon Ranger (EMR) is a fully-active tracking-calorimeter installed in the beam line of the Muon Ionization Cooling Experiment (MICE). The experiment will demonstrate ionization cooling, an essential technology needed for the…

The Muon Ionization Cooling Experiment (MICE) will perform a detailed study of ionization cooling to evaluate the feasibility of the technique. To carry out this program, MICE requires all of its detectors to reconstruct space points in a…

Instrumentation and Detectors · Physics 2018-05-18 F. Drielsma

Emittance exchange mediated by wedge absorbers can be used for longitudinal ionization cooling and for final transverse emittance minimization for a muon collider. A wedge absorber within the Muon Ionization Cooling Experiment (MICE) could…

Accelerator Physics · Physics 2018-06-06 Tanaz Angelina Mohayai , Pavel Snopok , David Neuffer , Don Summers

Muon colliders and neutrino factories are attractive options for future facilities aimed at achieving the highest lepton-antilepton collision energies and precision measurements of parameters of the Higgs boson and the neutrino mixing…

Accelerator Physics · Physics 2019-08-14 Daniel M. Kaplan

The Muon Ionization Cooling Experiment (MICE) will demonstrate the principle of muon beam phase-space reduction via ionization cooling. Muon beam cooling will be required for the proposed Neutrino Factory or Muon Collider. The phase-space…

Instrumentation and Detectors · Physics 2016-12-21 A. Dobbs , C. Hunt , K. Long , E. Santos , M. A. Uchida , P. Kyberd , C. Heidt , S. Blot , E. Overton

Small muon beams increase the luminosity of a muon collider. Reducing the momentum and position spreads of muons reduces emittance and leads to small, cool beams. Ionization cooling has been observed at the Muon Ionization Cooling…

High-brightness muon beams of energy comparable to those produced by state-of-the-art electron, proton and ion accelerators have yet to be realised. Such beams have the potential to carry the search for new phenomena in lepton-antilepton…

Accelerator Physics · Physics 2019-07-22 M. Bogomilov , R. Tsenov , G. Vankova-Kirilova , Y. P. Song , J. Y. Tang , Z. H. Li , R. Bertoni , M. Bonesini , F. Chignoli , R. Mazza , V. Palladino , A. de Bari , D. Orestano , L. Tortora , Y. Kuno , H. Sakamoto , A. Sato , S. Ishimoto , M. Chung , C. K. Sung , F. Filthaut , D. Jokovic , D. Maletic , M. Savic , N. Jovancevic , J. Nikolov , M. Vretenar , S. Ramberger , R. Asfandiyarov , A. Blondel , F. Drielsma , Y. Karadzhov , G. Charnley , N. Collomb , K. Dumbell , A. Gallagher , A. Grant , S. Griffiths , T. Hartnett , B. Martlew , A. Moss , A. Muir , I. Mullacrane , A. Oates , P. Owens , G. Stokes , P. Warburton , C. White , D. Adams , V. Bayliss , J. Boehm , T. W. Bradshaw , C. Brown , M. Courthold , J. Govans , M. Hills , J. -B. Lagrange , C. Macwaters , A. Nichols , R. Preece , S. Ricciardi , C. Rogers , T. Stanley , J. Tarrant , M. Tucker , S. Watson , A. Wilson , R. Bayes , J. C. Nugent , F. J. P. Soler , R. Gamet , P. Cooke , V. J. Blackmore , D. Colling , A. Dobbs , P. Dornan , P. Franchini , C. Hunt , P. B. Jurj , A. Kurup , K. Long , J. Martyniak , S. Middleton , J. Pasternak , M. A. Uchida , J. H. Cobb , C. N. Booth , P. Hodgson , J. Langlands , E. Overton , V. Pec , P. J. Smith , S. Wilbur , G. T. Chatzitheodoridis , A. J. Dick , K. Ronald , C. G. Whyte , A. R. Young , S. Boyd , J. R. Greis , T. Lord , C. Pidcott , I. Taylor , M. Ellis , R. B. S. Gardener , P. Kyberd , J. J. Nebrensky , M. Palmer , H. Witte , D. Adey , A. D. Bross , D. Bowring , P. Hanlet , A. Liu , D. Neuffer , M. Popovic , P. Rubinov , A. DeMello , S. Gourlay , A. Lambert , D. Li , T. Luo , S. Prestemon , S. Virostek , B. Freemire , D. M. Kaplan , T. A. Mohayai , P. Snopok , Y. Torun , L. M. Cremaldi , D. A. Sanders , D. J. Summers , L. R. Coney , G. G. Hanson , C. Heidt

Charged-particle tracking in the international Muon Ionisation Cooling Experiment (MICE) will be performed using two solenoidal spectrometers, each instrumented with a tracking detector based on 350 {\mu}m diameter scintillating fibres. The…