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Related papers: Project X: A Flexible High Power Proton Facility

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As part of the Intensity Frontier effort within the 2013 Community Summer Study, a workshop on the proton machine capabilities was held (High Intensity Secondary Beams Driven by Proton Beams) April 17-20, 2013 at Brookhaven National…

Accelerator Physics · Physics 2013-08-23 John Galambos , Mei Bai , Sergei Nagaitsev

We outline in detail a staging scenario for realizing the Neutrino Factory and the Muon Collider. As a first stage we envisage building an intense proton source that can be used to perform high intensity conventional neutrino beam…

High Energy Physics - Experiment · Physics 2019-08-17 Rajendran Raja , D. Cline , J. Gallardo , S. Geer , D. Kaplan , K. McDonald , R. Palmer , A. Sessler , A. N. Skrinsky , D. Summers , M. Tigner , A. Tollestrup , J. Wurtele , M. Zisman

The MINOS experiment at Fermilab has released an updated result on muon disappearance based upon 2.5 x 10^20 protons on target. The experiment utilizes the intense source of muon neutrinos provided by the NuMI beam line. This note…

High Energy Physics - Experiment · Physics 2019-08-13 Sacha E. Kopp

The completion of the PIP-II project and its superconducting linear accelerator will provide up to 1.2 MW of beam power to the LBNF/DUNE facility for neutrino physics. It will also be able to produce high-power beams directly from the linac…

One of the goals of the PXIE program at Fermilab is to demonstrate the capability to form an arbitrary bunch pattern from an initially CW 162.5 MHz H- bunch train coming out of an RFQ. The bunch-by-bunch selection will take place in the 2.1…

Accelerator Physics · Physics 2015-02-14 A. Shemyakin , C. Baffes

The Proton Improvement Plan-II (PIP-II) [1] has been developed at Fermilab to provide powerful proton beams to the laboratorys experiments. An 800-MeV superconducting linear accelerator-a centerpiece of the project-is currently under…

Accelerator Physics · Physics 2023-01-23 Igor Rakhno , Nikolai Mokhov , Igor Tropin , Sergei Striganov , Yury Eidelman

In recent years, the interest in high intensity proton beams in excess of several milli-Amperes has risen. Potential applications are in neutrino physics, materials and energy research, and isotope production. Continuous wave proton beams…

The bulk irradiation of materials with 10-30 MeV protons promises to advance the study of radiation damage for fission and fusion power plants. Intermediate energy proton beams can now be dedicated to materials irradiation within…

Fermilab operates the world's most intense antiproton source. Newly proposed experiments can use those antiprotons either parasitically during Tevatron Collider running or after the Tevatron Collider finishes in about 2010. In particular,…

High Energy Physics - Experiment · Physics 2008-10-19 Daniel M. Kaplan

The NuMI facility at Fermilab will provide an extremely intense beam of neutrinos for the MINOS neutrino-oscillation experiment. The spacious and fully-outfitted MINOS near detector hall will be the ideal venue for a high-statistics,…

High Energy Physics - Experiment · Physics 2012-08-27 Minerva Collaboration

Fermilab's Superconducting RF Beam Test Facility currently under construction will produce electron beams capable of damaging the acceleration structures and the beam line vacuum chambers in the event of an aberrant accelerator pulse. The…

Accelerator Physics · Physics 2012-10-01 A. Warner , L. Carmichael , M. Church , R. Neswold

Fermilab is committed to upgrade its accelerator complex to support HEP experiments at the intensity frontier. The ongoing Proton Improvement Plan (PIP) enables us to reach 700 kW beam power on the NuMI neutrino targets. By the end of the…

Accelerator Physics · Physics 2017-04-27 C. M. Bhat

Fermilab operates the world's most intense antiproton source, now exclusively dedicated to serving the needs of the Tevatron Collider. The anticipated 2009 shutdown of the Tevatron presents the opportunity for world-leading low- and…

High Energy Physics - Experiment · Physics 2007-07-16 Daniel M. Kaplan

FLASHForward is an experimental facility at DESY dedicated to beam-driven plasma-accelerator research. The X-2 experiment aims to demonstrate acceleration with simultaneous beam-quality preservation and high energy efficiency in a compact…

We sketch a staged plan for a series of muon-based facilities that can do compelling physics at each stage. Such a plan is unique in its ability to span both the Intensity and Energy Frontiers as defined by the P5 sub-panel of the US High…

Accelerator Physics · Physics 2019-08-13 Daniel M. Kaplan

NEXT is a high-pressure (10-15 bar) xenon Time Projection Chamber dedicated to neutrinoless double beta decay searches. NEXT-DEMO is a large prototype of the NEXT experiment, constructed to demonstrate the feasibility of the NEXT detector…

Instrumentation and Detectors · Physics 2019-08-13 Paola Ferrario

An outline is explained for hadron-physics projects at J-PARC, which is considered to be one of the flagship facilities in hadron physics from 2008. The facility provides an intensity frontier with 50 GeV proton beam for nuclear and…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Kumano

The nuSTORM facility has been designed to deliver beams of electron and muon neutrinos from the decay of a stored muon beam with a central momentum of 3.8 GeV/c and a momentum spread of 10%. The facility is unique in that it will: serve the…

Accelerator Physics · Physics 2013-05-08 D. Adey , S. K. Agarwalla , C. M. Ankenbrandt , R. Asfandiyarov , J. J. Back , G. Barker , E. Baussan , R. Bayes , S. Bhadra , V. Blackmore , A. Blondel , S. A. Bogacz , C. Booth , S. B. Boyd , A. Bravar , S. J. Brice , A. D. Bross , F. Cadoux , H. Cease , A. Cervera , J. Cobb , D. Colling , L. Coney , A. Dobbs , J. Dobson , A. Donini , P. J. Dornan , M. Dracos , F. Dufour , R. Edgecock , J. Evans , M. A. George , T. Ghosh , A. deGouvea , J. J. Gomez-Cadenas , A. Haesler , G. Hanson , M. Geelhoed , P. F. Harrison , M. Hartz , P. Hernandez , J. A. Hernando-Morata , P. J. Hodgson , P. Huber , A. Izmaylov , Y. Karadhzov , T. Kobilarcik , J. Kopp , L. Kormos , A. Korzenev , A. Kurup , Y. Kuno , P. Kyberd , J. P. Lagrange , A. M. Laing , J. Link , A. Liu , K. R. Long , N. McCauley , K. T. McDonald , K. Mahn , C. Martin , J. Martin , O. Mena , S. R. Mishra , N. Mokhov , J. Morfin , Y. Mori , W. Murray , D. Neuffer , R. Nichol , E. Noah , M. A. Palmer , S. Parke , S. Pascoli , J. Pasternak , M. Popovic , P. Ratoff , M. Ravonel , M. Rayner , S. Ricciardi , C. Rogers , P. Rubinov , E. Santos , A. Sato , E. Scantamburlo , J. K. Sedgbeer , D. R. Smith , P. J. Smith , J. T. Sobczyk , S. Soldner-Rembold , F. J. P. Soler , M. Sorel , A. Stahl , L. Stanco , P. Stamoulis , S. Striganov , H. Tanaka , I. J. Taylor , C. Touramanis , C. D. Tunnel , Y. Uchida , N. Vassilopoulos , M. O. Wascko , A. Weber , E. Wildner , M. J. Wilking , W. Winter , U. K. Yang

The peak current limit for the Fermilab Linac was recently studied. The purpose was to learn what components of the present Linac can be used for the first stage of a proposed proton driver[1]. For this application the Linac must provide a…

Accelerator Physics · Physics 2007-05-23 M. Popovic , L. Allen , A. Moretti , E. McCrory , C. W. Schmidt , T. Sullivan

The physics potential of an intense source of low-energy muons is studied. Such a source is a necessary stage towards building the neutrino factories and muon colliders which are being considered at present. The CERN Neutrino Factory could…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. Aysto , A. Baldini , A. Blondel , A. de Gouvea , J. Ellis , W. Fetscher , G. F. Giudice , K. Jungmann , S. Lola , V. Palladino , K. Tobe , A. Vacchi , A. van der Schaaf , K. Zuber
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