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Related papers: Producing an Intense, Cool Muon Beam via e+e- Anni…

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Tunneling electron-positron pair production is studied in a new setup in which a strong low-frequency and a weak high-frequency laser field propagate in the same direction and collide head-on with a relativistic nucleus. The…

High Energy Physics - Phenomenology · Physics 2009-10-29 A. Di Piazza , E. Lötstedt , A. I. Milstein , C. H. Keitel

Properties of some few-body systems which include one positively charged muon $\mu^{+}$ and two electrons $e^{-}$ are discussed. In particular, we consider the negatively charged muonium ion Mu$^{-}$ (or $\mu^{+} e^{-}_{2}$) and four-body…

Atomic Physics · Physics 2017-01-30 Alexei M Frolov

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…

In this paper, we investigate the production of a $\Xi^0 \bar{\Xi}^0$ using $e^+e^-$ collision data at ten center-of-mass energies between 3.51 and 4.95 GeV collected with the BESIII detector at the BEPCII collider and corresponding to an…

High Energy Physics - Phenomenology · Physics 2025-07-08 Azad I. Ahmadov

Muon ionization cooling is the only practical method for preparing high-brilliance beams needed for a neutrino factory or muon collider. The muon ionization cooling experiment (MICE) under development at the Rutherford Appleton Laboratory…

Accelerator Physics · Physics 2008-10-11 Alan D. Bross , Daniel M. kaplan

Recently, muon production in electron-proton scattering has been suggested as a possible candidate reaction for the identification of lepton-flavor violation due to physics beyond the Standard Model. Here we point out that the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Prashanth Jaikumar , Daniel R. Phillips , Lucas Platter , Madappa Prakash

We recall how a new light gauge boson emerged in Supersymmetric extensions of the Standard Model with an extra singlet superfield, and how it could behave very much as a light pseudoscalar, with the corresponding symmetry broken at a scale…

High Energy Physics - Phenomenology · Physics 2008-11-26 Pierre Fayet

Muon colliders are expected to naturally have a small spread in beam energy making them an ideal place to study the excitation curve. We present the parameter determinations that are possible from measuring the total cross section near…

High Energy Physics - Phenomenology · Physics 2009-10-30 M. S. Berger

Our goal is to investigate the charged Higgs phenomenology in the framework of 2HDM at the upcoming $e^+e^-$ and muon colliders. We are primarily concerned with the associated production processes with a fermion pair: $\ell^+ \ell^- \to…

High Energy Physics - Phenomenology · Physics 2024-09-02 Brahim Ait Ouazghour , Abdesslam Arhrib , Kingman Cheung , Es-said Ghourmin , Larbi Rahili

Producing valuable isotopes with high-flux high-energy neutrons generated by muon-catalyzed fusion ($\mu$CF) reactions could substantially improve the economic prospects for muon-catalyzed fusion. Because no external heating is required for…

Plasma Physics · Physics 2025-12-29 J. F. Parisi , A. Rutkowski

It is well known that at linear e^+e^-(e^-e^-) colliders using laser backscattering one can obtain colliding gamma-gamma, gamma-electron beams with energy and luminosity comparable to those in e^+e^- collisions. In this paper, it is…

High Energy Physics - Experiment · Physics 2016-08-31 Valery Telnov

We study the fluxes of anti-deuterons that could be produced by annihilations in the galactic halo of Dark Matter particles with multi-TeV mass and a large annihilation cross section, as indicated by the recent PAMELA results. The model of…

High Energy Physics - Phenomenology · Physics 2010-12-17 Carolin B. Braeuninger , Marco Cirelli

A large admittance sector cyclotron filled with LiH wedges surrounded by helium or hydrogen gas is explored. Muons are cooled as they spiral adiabatically into a central swarm. As momentum approaches zero, the momentum spread also…

Accelerator Physics · Physics 2009-11-11 D. J. Summers , S. B. Bracker , L. M. Cremaldi , R. Godang , R. B. Palmer

It has been suggested that the annihilation of Dark Matter particles \chi with mass between 0.5 and 20 MeV into e^+e^- pairs could be responsible for the excess flux of 511 keV photons coming from the central region of our galaxy that has…

High Energy Physics - Phenomenology · Physics 2008-11-26 Natalia Borodatchenkova , Debajyoti Choudhury , Manuel Drees

A scheme is proposed for the preparation of a tagged highly polarized antineutron beam, so far not available for experiments. Unpolarized antineutron fluxes are expected to exceed previous intensities by more than an order of magnitude. The…

Accelerator Physics · Physics 2010-12-08 Berthold Schoch

The neutrino induced hyperon production processes $\bar{\nu}_{e/\mu} + p \to e^+/\mu^+ + \pi + \Lambda/\Sigma$ may provide a unique clean place for studying low energy $\pi\Lambda/\Sigma$ interaction and hyperon resonances below $KN$…

High Energy Physics - Phenomenology · Physics 2015-04-14 Jia-Jun Wu , Bing-Song Zou

Generation of antimatter via the multiphoton Breit-Wheeler process in an all-optical scheme will be made possible on forthcoming high-power laser facilities through the collision of wakefield-accelerated GeV electrons with a…

Plasma Physics · Physics 2017-04-12 Mathieu Lobet , Xavier Davoine , Emmanuel d'Humières , Laurent Gremillet

A low-emittance, high-intensity atomic beam of muonium ($\mathrm{M}=\mu^+ + \mathrm{e}^-$) using superfluid helium as muon-to-muonium converter is being developed at the Paul Scherrer Institute (PSI). This beam could advance laser…

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

We consider the electromagnetic production of positron in collision of heavy nuclei, with the simultaneously produced electron captured by one of the nuclei. This cross-section exceeds by about four orders of magnitude the cross-section of…

Nuclear Theory · Physics 2016-06-27 I. B. Khriplovich , D. A. Solovyev