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The term beta-beam has been coined for the production of a pure beam of electron neutrinos or their antiparticles through the decay of radioactive ions circulating in a storage ring. This concept requires radioactive ions to be accelerated…

The 2020 Update of the European Strategy for Particle Physics (ESPP) (see https://cds.cern.ch/record/2720129 ) recommended that muon beam R\&D should be considered a high-priority future initiative and that a programme of experimentation be…

High Energy Physics - Experiment · Physics 2022-08-10 L. Alvarez Ruso , T. Alves , S. Boyd , A. Bross , P. R. Hobson , P. Kyberd , J. B. Lagrange , K. Long , X. -G. Lu , J. Pasternak , M. Pfaff , C. Rogers

Neutrino beam with about 300 MeV in energy, high-flux and medium baseline is considered a rational choice for measuring CP violation before the more powerful Neutrino Factory will be built. Following this concept, a unique neutrino beam…

This paper investigates the feasibility of re-purposing the MuCool Test Area (MTA) beamline and experimental hall to support a Muon Spin Resonance (MuSR) facility, which would make it the only such facility in the US. This report reviews…

Accelerator Physics · Physics 2018-06-13 John A. Johnstone , Carol Johnstone

There have been active efforts in the U.S., Europe, and Japan on the design of a Neutrino Factory. This type of facility produces intense beams of neutrinos from the decay of muons in a high energy storage ring. In the U.S., a second…

The recent discovery that neutrinos have masses opens a wide new field of experimentation. Accelerator-made neutrinos are essential in this program. Ideas for future facilities include high intensity muon neutrino beams from pion decay…

High Energy Physics - Phenomenology · Physics 2016-09-06 A. Blondel , A. Cervera-Villanueva , A. Donini , P. Huber , M. Mezzetto , P. Strolin

A new muon and pion capture system is proposed for the China Spallation Neutron Source (CSNS), currently under construction. Using about 4\% of the pulsed proton beam (1.6 GeV, 4 kW and 1 Hz) of CSNS to bombard a cylindrical graphite target…

Accelerator Physics · Physics 2016-08-03 Ran Xiao , Yanfen Liu , Wenzhen Xu , Xiaojie Ni , Ziwen Pan , Bangjiao Ye

We study the possibilities offered by muon storage rings for tau-neutrino appearance experiments due to nu_mu to nu_tau and nu_e to nu_tau oscillations. Tau event rates for such experiments are first discussed with a view to examining their…

High Energy Physics - Phenomenology · Physics 2009-01-07 Sukanta Dutta , Raj Gandhi , Biswarup Mukhopadhyaya

The Neutrinos at the Main Injector (NuMI) beamline will deliver an intense muon neutrino beam by focusing a beam of mesons into a long evacuated decay volume. The beam must be steered with 1 mRad angular accuracy toward the Soudan…

This paper describes the hardware and operations of the Neutrinos at the Main Injector (NuMI) beam at Fermilab. It elaborates on the design considerations for the beam as a whole and for individual elements. The most important design…

Accelerator Physics · Physics 2015-12-09 P. Adamson , K. Anderson , M. Andrews , R. Andrews , I. Anghel , D. Augustine , A. Aurisano , S. Avvakumov , D. S. Ayres , B. Baller , B. Barish , G. Barr , W. L. Barrett , R. H. Bernstein , J. Biggs , M. Bishai , A. Blake , V. Bocean , G. J. Bock , D. J. Boehnlein , D. Bogert , K. Bourkland , S. V. Cao , C. M. Castromonte , S. Childress , B. C. Choudhary , J. A. B. Coelho , J. H. Cobb , L. Corwin , D. Crane , J. P. Cravens , D. Cronin-Hennessy , R. J. Ducar , J. K. de Jong , A. V. Devan , N. E. Devenish , M. V. Diwan , A. R. Erwin , C. O. Escobar , J. J. Evans , E. Falk , G. J. Feldman , T. H. Fields , R. Ford , M. V. Frohne , H. R. Gallagher , V. Garkusha , R. A. Gomes , M. C. Goodman , P. Gouffon , N. Graf , R. Gran , N. Grossman , K. Grzelak , A. Habig , S. R. Hahn , D. Harding , D. Harris , P. G. Harris , J. Hartnell , R. Hatcher , S. Hays , K. Heller , A. Holin , J. Huang , J. Hylen , A. Ibrahim , D. Indurthy , G. M. Irwin , Z. Isvan , D. E. Jaffe , C. James , D. Jensen , J. Johnstone , T. Kafka , S. M. S. Kasahara , G. Koizumi , S. Kopp , M. Kordosky , A. Kreymer , K. Lang , C. Laughton , G. Lefeuvre , J. Ling , P. J. Litchfield , L. Loiacono , P. Lucas , W. A. Mann , A. Marchionni , M. L. Marshak , N. Mayer , C. McGivern , M. M. Medeiros , R. Mehdiyev , J. R. Meier , M. D. Messier , D. G. Michael , R. H. Milburn , J. L. Miller , W. H. Miller , S. R. Mishra , S. Moed Sher , C. D. Moore , J. Morfin , L. Mualem , S. Mufson , S. Murgia , M. Murtagh , J. Musser , D. Naples , J. K. Nelson , H. B. Newman , R. J. Nichol , J. A. Nowak , J. O Connor , W. P. Oliver , M. Olsen , M. Orchanian , S. Osprey , R. B. Pahlka , J. Paley , A. Para , R. B. Patterson , T. Patzak , Z. Pavlovic , G. Pawloski , A. Perch , E. A. Peterson , D. A. Petyt , M. M. Pfutzner , S. Phan-Budd , R. K. Plunkett , N. Poonthottathil , P. Prieto , D. Pushka , X. Qiu , A. Radovic , R. A. Rameika , J. Ratchford , B. Rebel , R. Reilly , C. Rosenfeld , H. A. Rubin , K. Ruddick , M. C. Sanchez , N. Saoulidou , L. Sauer , J. Schneps , D. Schoo , A. Schreckenberger , P. Schreiner , P. Shanahan , R. Sharma , W. Smart , C. Smith , A. Sousa , A. Stefanik , N. Tagg , R. L. Talaga , G. Tassotto , J. Thomas , J. Thompson , M. A. Thomson , X. Tian , A. Timmons , D. Tinsley , S. C. Tognini , R. Toner , D. Torretta , I. Trostin , G. Tzanakos , J. Urheim , P. Vahle , K. Vaziri , E. Villegas , B. Viren , G. Vogel , R. C. Webber , A. Weber , R. C. Webb , A. Wehmann , C. White , L. Whitehead , L. H. Whitehead , S. G. Wojcicki , M. L. Wong-Squires , T. Yang , F. X. Yumiceva , V. Zarucheisky , R. Zwaska

Muon storage rings have been proposed for use as a source of high-energy neutrino beams (the Neutrino Factory) and as the basis for a high-energy lepton-antilepton collider (the Muon Collider). The Neutrino Factory is widely believed to be…

Accelerator Physics · Physics 2007-07-16 D. M. Kaplan , K. Long

We discuss the design of the muon capture front end for a \mu+-\mu- Collider. In the front end, a proton bunch on a target creates secondary pions that drift into a capture transport channel, decaying into muons. A sequence of rf cavities…

Accelerator Physics · Physics 2012-02-27 D. Neuffer , C. Yoshikawa

The muEDM experiment at the Paul Scherrer Institute aims to measure the electric dipole moment with an unprecedented sensitivity of $6 \times 10^{-23}\,\mathrm{e}\cdot\mathrm{cm}$. A key aspect of this experiment is the injection and…

An extension of the TRIUMF M13 low-energy pion channel designed to suppress positrons based on an energy-loss technique is described. A source of beam channel momentum calibration from the decay pi+ --> e+ nu is also described.

The (International Design Report) IDR neutrino factory scenario for capture, bunching, phase-energy rotation and initial cooling of micro's produced from a proton source target is explored. It requires a drift section from the target, a…

Accelerator Physics · Physics 2015-06-04 David Neuffer , Gersende Prior , Christopher Rogers , Pavel Snopok , Cary Yoshikawa

The EUROnu project has studied three possible options for future, high intensity neutrino oscillation facilities in Europe. The first is a Super Beam, in which the neutrinos come from the decay of pions created by bombarding targets with a…

Accelerator Physics · Physics 2013-05-20 T. R. Edgecock , O. Caretta , T. Davenne , C. Densham , M. Fitton , D. Kelliher , P. Loveridge , S. Machida , C. Prior , C. Rogers , M. Rooney , J. Thomason , D. Wilcox , E. Wildner , I. Efthymiopoulos , R. Garoby , S. Gilardoni , C. Hansen , E. Benedetto , E. Jensen , A. Kosmicki , M. Martini , J. Osborne , G. Prior , T. Stora , T. Melo-Mendonca , V. Vlachoudis , C. Waaijer , P. Cupial , A. Chancé , A. Longhin , J. Payet , M. Zito , E. Baussan , C. Bobeth , E. Bouquerel , M. Dracos , G. Gaudiot , B. Lepers , F. Osswald , P. Poussot , N. Vassilopoulos , J. Wurtz , V. Zeter , J. Bielski , M. Kozien , L. Lacny , B. Skoczen , B. Szybinski , A. Ustrycka , A. Wroblewski , M. Marie-Jeanne , P. Balint , C. Fourel , J. Giraud , J. Jacob , T. Lamy , L. Latrasse , P. Sortais , T. Thuillier , S. Mitrofanov , M. Loiselet , Th. Keutgen , Th. Delbar , F. Debray , C. Trophine , S. Veys , C. Daversin , V. Zorin , I. Izotov , V. Skalyga , G. Burt , A. C. Dexter , V. L. Kravchuk , T. Marchi , M. Cinausero , F. Gramegna , G. De Angelis , G. Prete , G. Collazuol , M. Laveder , M. Mazzocco , M. Mezzetto , C. Signorini , E. Vardaci , A. Di Nitto , A. Brondi , G. La Rana , P. Migliozzi , R. Moro , V. Palladino , N. Gelli , D. Berkovits , M. Hass , T. Y. Hirsh , M. Schaumann , A. Stahl , J. Wehner , A. Bross , J. Kopp , D. Neuffer , R. Wands , R. Bayes , A. Laing , P. Soler , S. K. Agarwalla , A. Cervera Villanueva , A. Donini , T. Ghosh , J. J. Gómez Cadenas , P. Hernández , J. Martín-Albo , O. Mena , J. Burguet-Castell , L. Agostino , M. Buizza-Avanzini , M. Marafini , T. Patzak , A. Tonazzo , D. Duchesneau , L. Mosca , M. Bogomilov , Y. Karadzhov , R. Matev , R. Tsenov , E. Akhmedov , M. Blennow , M. Lindner , T. Schwetz , E. Fernández Martinez , M. Maltoni , J. Menéndez , C. Giunti , M. C. González García , J. Salvado , P. Coloma , P. Huber , T. Li , J. López-Pavón , C. Orme , S. Pascoli , D. Meloni , J. Tang , W. Winter , T. Ohlsson , H. Zhang , L. Scotto-Lavina , F. Terranova , M. Bonesini , L. Tortora , A. Alekou , M. Aslaninejad , C. Bontoiu , A. Kurup , L. J. Jenner , K. Long , J. Pasternak , J. Pozimski , J. J. Back , P. Harrison , K. Beard , A. Bogacz , J. S. Berg , D. Stratakis , H. Witte , P. Snopok , N. Bliss , M. Cordwell , A. Moss , S. Pattalwar , M. Apollonio

We present FLUKA and MARS simulation studies of the pion production and energy deposition in the Neutrino Factory baseline target station, which consists of a 4 MW proton beam interacting with a liquid mercury jet target within a 20 T…

Accelerator Physics · Physics 2013-03-08 John J. Back , Chris Densham , Rob Edgecock , Gersende Prior

A Neutrino Factory producing an intense beam composed of nu_e(nubar_e) and nubar_mu(nu_mu) from muon decays has been shown to have the greatest sensitivity to the two currently unmeasured neutrino mixing parameters, theta_13 and delta_CP .…

High Energy Physics - Experiment · Physics 2015-03-13 A. Cervera , A. Laing , J. Martin-Albo , F. J. P. Soler

Storage rings have been employed over three decades in various kinds of nuclear and atomic physics experiments with highly charged ions. Storage ring operation and precision physics experiments benefit from the availability of beam cooling…

Nuclear Experiment · Physics 2020-10-28 Markus Steck , Yuri A. Litvinov