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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

Conceptual design studies are underway for muon colliders and other high-current muon storage rings that have the potential to become the first true ``neutrino factories''. Muon decays in long straight sections of the storage rings would…

High Energy Physics - Phenomenology · Physics 2010-05-28 I. Bigi , T. Bolton , J. Formaggio , D. A. Harris , B. Kayser , B. J. King , K. S. McFarland , J. Morfin , A. A. Petrov , H. Schellman , R. Shrock , P. G. Spentzouris , M. Velasco , J. Yu

Muon colliders provide an exciting new direction to expand the energy frontier of particle physics. We point out a new use of these facilities for neutrino and beyond the Standard Model physics using their main detectors. Muon decays along…

High Energy Physics - Phenomenology · Physics 2025-07-31 Luc Bojorquez-Lopez , Matheus Hostert , Carlos A. Argüelles , Zhen Liu

The potential of muon colliders to address fundamental physics issues is explored, with emphasis on understanding the nature of electroweak symmetry breaking. The $s$-channel production of Higgs bosons, unique to a muon collider, along with…

High Energy Physics - Phenomenology · Physics 2009-10-31 V. Barger

The Proton Improvement Plan II (PIPII) is a superconducting linear accelerator being built at Fermilab that will provide 800 MeV proton beams for neutrino production. The Linac requires cooling at 80 K, 5 K, and 2 K temperatures, which will…

Accelerator Physics · Physics 2022-06-23 Ashish Kumar Shukla , Andrew Dalesandro , Ram Dhuley , William Soyars

New strong dynamics at the energy scale ~ 1 TeV is an attractive and elegant theoretical ansatz for the origin of electroweak symmetry breaking. We review here the theoretical models for strong dynamics, particularly, technicolor theories…

High Energy Physics - Phenomenology · Physics 2009-10-31 Pushpalatha Bhat , Estia Eichten

This paper describes a new way to reconstruct and identify muons with high efficiency and high pion rejection. Since muons at the ILC are often produced with or in jets, for many of the physics channels of interest[1], an efficient…

Instrumentation and Detectors · Physics 2015-06-26 C. Milstene , G. Fisk , A. Para

Project-X is the proposed high intensity proton facility to be built at Fermilab, US. Its Superconducting Linac, to be used at first stage of acceleration, will be operated in continuous wave (CW) mode. The Linac is divided into three…

Accelerator Physics · Physics 2012-02-27 A. Saini , K. Ranjan , N. Solyak , S. Mishra , V. Yakovlev

We have explored a concept for an advanced Normal-Conducting Radio-Frequency (NCRF) C-band linear accelerator (linac) structure to achieve a high gradient, high power e$^+$e$^-$ linear collider in the TeV class. This design study represents…

A multi-TeV muon collider offers a spectacular opportunity in the direct exploration of the energy frontier. Offering a combination of unprecedented energy collisions in a comparatively clean leptonic environment, a high energy muon…

High Energy Physics - Experiment · Physics 2023-08-10 K. M. Black , S. Jindariani , D. Li , F. Maltoni , P. Meade , D. Stratakis , D. Acosta , R. Agarwal , K. Agashe , C. Aime , D. Ally , A. Apresyan , A. Apyan , P. Asadi , D. Athanasakos , Y. Bao , E. Barzi , N. Bartosik , L. A. T. Bauerdick , J. Beacham , S. Belomestnykh , J. S. Berg , J. Berryhill , A. Bertolin , P. C. Bhat , M. E. Biagini , K. Bloom , T. Bose , A. Bross , E. Brost , N. Bruhwiler , L. Buonincontri , D. Buttazzo , V. Candelise , A. Canepa , L. Carpenter , M. Casarsa , F. Celiberto , C. Cesarotti , G. Chachamis , Z. Chacko , P. Chang , S. V. Chekanov , T. Y. Chen , M. Chiesa , T. Cohen , M. Costa , N. Craig , A. Crivellin , C. Curatolo , D. Curtin , G. Da Molin , S. Dasu , A. de Gouvea , D. Denisov , R. Dermisek , K. F. Di Petrillo , T. Dorigo , J. M. Duarte , V. D. Elvira , R. Essig , P. Everaerts , J. Fan , M. Felcini , G. Fiore , D. Fiorina , M. Forslund , R. Franceschini , M. V. Garzelli , C. E. Gerber , L. Giambastiani , D. Giove , S. Guiducci , T. Han , K. Hermanek , C. Herwig , J. Hirschauer , T. R. Holmes , S. Homiller , L. A. Horyn , A. Ivanov , B. Jayatilaka , H. Jia , C. K. Jung , Y. Kahn , D. M. Kaplan , M. Kaur , M. Kawale , P. Koppenburg , G. Krintiras , K. Krizka , B. Kuchma , L. Lee , L. Li , P. Li , Q. Li , W. Li , R. Lipton , Z. Liu , S. Lomte , Q. Lu , D. Lucchesi , T. Luo , K. Lyu , Y. Ma , P. A. N. Machado , C. Madrid , D. J. Mahon , A. Mazzacane , N. McGinnis , C. McLean , B. Mele , F. Meloni , S. C. Middleton , R. K. Mishra , N. Mokhov , A. Montella , M. Morandin , S. Nagaitsev , F. Nardi , M. S. Neubauer , D. V. Neuffer , H. Newman , R. Ogaz , I. Ojalvo , I. Oksuzian , T. Orimoto , B. Ozek , K. Pachal , S. Pagan Griso , P. Panci , V. Papadimitriou , N. Pastrone , K. Pedro , F. Pellemoine , A. Perloff , D. Pinna , F. Piccinini , Marc-Andre Pleier , S. Posen , K. Potamianos , S. Rappoccio , M. Reece , L. Reina , A. Reinsvold Hall , C. Riccardi , L. Ristori , T. Robens , R. Ruiz , P. Sala , D. Schulte , L. Sestini , V. Shiltsev , P. Snopok , G. Stark , J. Stupak , S . Su , R. Sundrum , M. Swiatlowski , M. J. Syphers , A. Taffard , W. Thompson , Y. Torun , C. G. Tully , I. Vai , M. Valente , U. van Rienen , R. van Weelderen , G. Velev , N. Venkatasubramanian , L. Vittorio , C. Vuosalo , X. Wang , H. Weber , R. Wu , Y. Wu , A. Wulzer , K. Xie , S. Xie , R. Yohay , K. Yonehara , F. Yu , A. V. Zlobin , D. Zuliani , J. Zurita

The demand for neutron production facilities is increasing, as the applications of neutron science are manifold. These applications drive the need for efficient and compact neutron sources. In this context, this paper explores the potential…

The China spallation neutron source (CSNS) linac is designed with beam energy of 81MeV and a peak current of 15mA in the first phase. The RF power system for the 81 MeV Linac requires 8 units of RF power sources, each unit has one…

Accelerator Physics · Physics 2019-09-26 Linyan Rong , Zhencheng Mu , Zhexin Xie , Bo Wang , Wenzhong Zhou , Maliang Wan , Meifei Liu , Jian Li , Xinan Xu

A muon collider is expected to produce a high intensity neutrino beam which is an admixture of either $\nu_{\mu}+\bar{\nu_e}$ or $\bar{\nu}_{\mu} +\nu_e$ which can can be directed to underground detectors far away from the source. It will…

High Energy Physics - Phenomenology · Physics 2011-07-19 R. N. Mohapatra

As the pre-injector of the LHC injector chain, the proton linac at CERN is required to provide a high-intensity (180mA) beam to the Proton Synchrotron Booster. The results of measurements at this intensity will be presented. Furthermore,…

Accelerator Physics · Physics 2007-05-23 C. E. Hill , A. Lombardi , R. Scrivens , M. Vretenar , A. Feschenko , A. Liou

A superconducting double spin valve device is proposed. Its operation takes advantage of the interplay between the spin-filtering effect of ferromagnetic insulators and superconductivity-induced out-of-equilibrium transport. Depending on…

Mesoscale and Nanoscale Physics · Physics 2009-08-03 Francesco Giazotto

One of the key systems of a Muon Collider (MC) - seen as the most exciting option for the energy frontier machine in the post-LHC era - is its interaction region (IR). Designs of its optics, magnets and machine-detector interface are…

Accelerator Physics · Physics 2012-02-20 N. V. Mokhov , Y. I. Alexahin , V. V. Kashikhin , S. I. Striganov , A. V. Zlobin

The surprising discovery of superconductivity in layered iron-based materials, with transition temperatures climbing as high as 55 K, has lead to thousands of publications on this subject over the past two years. While there is general…

Superconductivity · Physics 2010-09-16 Johnpierre Paglione , Richard L. Greene

The search for superconductivity in materials iso-structural and iso-valent with magnesium diboride, MgB2, has not yielded any results close enough to the 39K Tc of MgB2. Lithium magnesium nitride, LiMgN, resembles MgB2 in that they both…

Superconductivity · Physics 2012-04-25 O. P. Isikaku-Ironkwe

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

Superconducting nanowires can be fabricated by decomposition of an organometallic gas using a focused beam of Ga ions. However, physical damage and unintentional doping often results from the exposure to the ion beam, motivating the search…

Mesoscale and Nanoscale Physics · Physics 2015-02-18 Shamashis Sengupta , Chuan Li , Cedric Baumier , Alik Kasumov , S. Gueron , H. Bouchiat , F. Fortuna
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