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Emittance exchange mediated by wedge absorbers is required for longitudinal ionization cooling and for final transverse emittance minimization for a muon collider. A wedge absorber within the MICE beam line could serve as a demonstration of…

Accelerator Physics · Physics 2016-12-23 David Neuffer , J. Acosta , D. Summers , T. Mohayai , P. Snopok

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

The Muon Ionization Cooling Experiment (MICE) will demonstrate the feasibility of ionization cooling, the technique by which it is proposed to cool the muon beam at a future neutrino factory or muon collider. The position and momentum…

Accelerator Physics · Physics 2018-06-13 Durga Rajaram , Victoria Blackmore

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

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

Experiments with muons ($\mu^{+}$) and muonium atoms ($\mu^{+}e^{-}$) offer several promising possibilities for testing fundamental symmetries. Examples of such experiments include search for muon electric dipole moment, measurement of muon…

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

A new scheme to produce very low emittance muon beams using a positron beam of about 45~GeV interacting on electrons on target is presented. One of the innovative topics to be investigated is the behaviour of the positron beam stored in a…

Accelerator Physics · Physics 2018-08-01 M. Boscolo , M. Antonelli , O. R. Blanco-Garcia , S. Guiducci , S. Liuzzo , P. Raimondi , F. Collamati

A novel device to compress the phase space of a muon beam by a factor of $10^{10}$ with a $10^{-3}$ efficiency is under development. A surface muon beam is stopped in a helium gas target consisting of several compression stages, wherein…

Possible application for muon experiments such as mu2e is discussed of the initial part of the ionization cooling channel originally developed for muon collider. It is shown that with the FNAL Booster as the proton driver the mu2e…

Accelerator Physics · Physics 2014-09-22 Y. Alexahin , D. Neuffer , E. Prebys

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 2021-08-18 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 , V. Palladino , 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 , 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 , D. Rajaram , P. Snopok , Y. Torun , L. M. Cremaldi , D. A. Sanders , D. J. Summers , L. R. Coney , G. G. Hanson , C. Heidt

The relative immunity of muons to synchrotron radiation suggests that they might be used in place of electrons as probes in fundamental high-energy physics experiments. Muons are commonly produced indirectly through pion decay by…

Accelerator Physics · Physics 2015-04-03 Diktys Stratakis , David V. Neuffer

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

Low-energy muon beams are useful for a range of physics experiments. We consider the production of low-energy muon beams with small energy spreads using frictional cooling. As the input beam, we take a surface muon source such as that at…

Accelerator Physics · Physics 2015-05-18 Yu Bao , Allen Caldwell , Daniel Greenwald , Guoxing Xia

Muon beams of low emittance provide the basis for the intense, well-characterised neutrino beams necessary to elucidate the physics of flavour at a neutrino factory and to provide lepton-antilepton collisions at energies of up to several…

Accelerator Physics · Physics 2017-06-28 MICE Collaboration , M. Bogomilov , R. Tsenov , G. Vankova-Kirilova , Y. Song , J. Tang , Z. Li , R. Bertoni , M. Bonesini , F. Chignoli , R. Mazza , V. Palladino , A. de Bari , G. Cecchet , D. Orestano , L. Tortora , Y. Kuno , S. Ishimoto , F. Filthaut , D. Jokovic , D. Maletic , M. Savic , O. M. Hansen , S. Ramberger , M. Vretenar , R. Asfandiyarov , A. Blondel , F. Drielsma , Y. Karadzhov , G. Charnley , N. Collomb , A. Gallagher , A. Grant , S. Griffiths , T. Hartnett , B. Martlew , A. Moss , A. Muir , I. Mullacrane , A. Oates , P. Owens , G. Stokes , M. Tucker , P. Warburton , C. White , D. Adams , R. J. Anderson , P. Barclay , V. Bayliss , J. Boehm , T. W. Bradshaw , M. Courthold , K. Dumbell , V. Francis , L. Fry , T. Hayler , M. Hills , A. Lintern , C. Macwaters , A. Nichols , R. Preece , S. Ricciardi , C. Rogers , T. Stanley , J. Tarrant , A. Wilson , S. Watson , R. Bayes , J. C. Nugent , F. J. P. Soler , R. Gamet , G. Barber , V. J. Blackmore , D. Colling , A. Dobbs , P. Dornan , C. Hunt , A. Kurup , J-B. Lagrange , K. Long , J. Martyniak , S. Middleton , J. Pasternak , M. A. Uchida , J. H. Cobb , W. Lau , C. N. Booth , P. Hodgson , J. Langlands , E. Overton , M. Robinson , P. J. Smith , S. Wilbur , A. J. Dick , K. Ronald , C. G. Whyte , A. R. Young , S. Boyd , P. Franchini , J. R. Greis , C. Pidcott , I. Taylor , R. B. S. Gardener , P. Kyberd , J. J. Nebrensky , M. Palmer , H. Witte , A. D. Bross , D. Bowring , A. Liu , D. Neuffer , M. Popovic , P. Rubinov , A. DeMello , S. Gourlay , D. Li , S. Prestemon , S. Virostek , B. Freemire , P. Hanlet , D. M. Kaplan , T. A. Mohayai , D. Rajaram , P. Snopok , V. Suezaki , Y. Torun , Y. Onel , L. M. Cremaldi , D. A. Sanders , D. J. Summers , G. G. Hanson , C. Heidt

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…

Wedge absorbers are needed to obtain longitudinal cooling in ionization cooling. They also can be used to obtain emittance exchanges between longitudinal and transverse phase space. There can be large exchanges in emittance, even with…

Accelerator Physics · Physics 2017-09-14 David Neuffer , D. Summers , T. Mohayai , P. Snopok , C. Rogers

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

Low-energy muon beams are useful for rare decay searches, which provide access to new physics that cannot be addressed at high-energy colliders. However, muons are produced within a broad energy spread unmatched to the low-energy required.…

Accelerator Physics · Physics 2016-07-04 D. Neuffer , Y. Bao , G. Hansen

The Muon Ionization Cooling Experiment (MICE) collaboration seeks to demonstrate the feasibility of ionization cooling, the technique by which it is proposed to cool the muon beam at a future neutrino factory or muon collider. The emittance…

Accelerator Physics · Physics 2019-03-27 The MICE Collaboration , D. Adams , D. Adey , R. Asfandiyarov , G. Barber , A. de Bari , R. Bayes , V. Bayliss , R. Bertoni , V. Blackmore , A. Blondel , J. Boehm , M. Bogomilov , M. Bonesini , C. N. Booth , D. Bowring , S. Boyd , T. W. Bradshaw , A. D. Bross , C. Brown , L. Coney , G. Charnley , G. T. Chatzitheodoridis , F. Chignoli , M. Chung , D. Cline , J. H. Cobb , D. Colling , N. Collomb , P. Cooke , M. Courthold , L. M. Cremaldi , A. DeMello , A. J. Dick , A. Dobbs , P. Dornan , F. Drielsma , K. Dumbell , M. Ellis , F. Filthaut , P. Franchini , B. Freemire , A. Gallagher , R. Gamet , R. B. S. Gardener , S. Gourlay , A. Grant , J. R. Greis , S. Griffiths , P. Hanlet , G. G. Hanson , T. Hartnett , C. Heidt , P. Hodgson , C. Hunt , S. Ishimoto , D. Jokovic , P. B. Jurj , D. M. Kaplan , Y. Karadzhov , A. Klier , Y. Kuno , A. Kurup , P. Kyberd , J-B. Lagrange , J. Langlands , W. Lau , D. Li , Z. Li , A. Liu , K. Long , T. Lord , C. Macwaters , D. Maletic , B. Martlew , J. Martyniak , R. Mazza , S. Middleton , T. A. Mohayai , A. Moss , A. Muir , I. Mullacrane , J. J. Nebrensky , D. Neuffer , A. Nichols , J. C. Nugent , A. Oates , D. Orestano , E. Overton , P. Owens , V. Palladino , M. Palmer , J. Pasternak , V. Pec , C. Pidcott , M. Popovic , R. Preece , S. Prestemon , D. Rajaram , S. Ricciardi , M. Robinson , C. Rogers , K. Ronald , P. Rubinov , H. Sakamoto , D. A. Sanders , A. Sato , M. Savic , P. Snopok , P. J. Smith , F. J. P. Soler , Y. Song , T. Stanley , G. Stokes , V. Suezaki , D. J. Summers , C. K. Sung , J. Tang , J. Tarrant , I. Taylor , L. Tortora , Y. Torun , R. Tsenov , M. Tucker , M. A. Uchida , S. Virostek , G. Vankova-Kirilova , P. Warburton , S. Wilbur , A. Wilson , H. Witte , C. White , C. G. Whyte , X. Yang , A. R. Young , M. Zisman
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