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

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In response to the growing interest in building a Neutrino Factory to produce high intensity beams of electron- and muon-neutrinos and antineutrinos, in October 1999 the Fermilab Directorate initiated two six-month studies. The first study,…

The Project X Injector Experiment (PXIE), a test bed for the Project X front end, will be completed at Fermilab at FY12-16. One of the challenging goals of PXIE is demonstration of the capability to form a 1 mA H- beam with an arbitrary…

Fermilab is planning the construction of a prototype front end of the Project X linac. The Project X Injector Experiment (PXIE) is expected to accelerate 1 mA cw H- beam up to 30 MeV. Some of the major goals of the project are to test a cw…

Accelerator Physics · Physics 2013-01-30 V. A. Lebedev , A. V. Shemyakin , J. Steimel , M. Wendt , B. M. Hanna , L. R. Prost , V. E. Scarpine

High energy and high beam power accelerators are extensively used for the neutrino physics research. At present, the leading operational facilities are the Fermilab Main Injector complex that delivers over 0.75 MW of 120 GeV protons on the…

Accelerator Physics · Physics 2019-06-19 Vladimir Shiltsev

The Proton Improvement Plan II (PIP-II) at Fermilab is a program of upgrades to the injection complex. At its core is the design and construction of a CW-compatible, pulsed H- superconducting RF linac. To validate the concept of the…

Accelerator Physics · Physics 2015-11-05 L. Prost , M. Alvarez , R. Andrews , J. -P. Carneiro , B. Hanna , V. Scarpine , A. Shemyakin , R. D'Arcy , C. Wiesner

The Long Baseline Neutrino Experiment (LBNE) will utilize a neutrino beamline facility located at Fermilab to carry out a compelling research program in neutrino physics. The facility will aim a beam of neutrinos toward a detector placed at…

Accelerator Physics · Physics 2013-01-30 R. Andrews , A. Z. Chen , S. C. Childress , C. D. Moore , V. Papadimitriou , M. R. Campbell

Project-X is the proposed high intensity proton facility to be built at Fermilab, US. First stage of the Project-X consists of superconducting linac which will be operated in continuous wave (CW) mode to accelerate the beam from 2.5 MeV to…

Accelerator Physics · Physics 2012-03-08 A. Saini , K. Ranjan , N. Solyak , S. Mishra , V. Yakovlev

Part 2 of "Project X: Accelerator Reference Design, Physics Opportunities, Broader Impacts". In this Part, we outline the particle-physics program that can be achieved with Project X, a staged superconducting linac for intensity-frontier…

High Energy Physics - Experiment · Physics 2016-10-04 Andreas S. Kronfeld , Robert S. Tschirhart , Usama Al-Binni , Wolfgang Altmannshofer , Charles Ankenbrandt , Kaladi Babu , Sunanda Banerjee , Matthew Bass , Brian Batell , David V. Baxter , Zurab Berezhiani , Marc Bergevin , Robert Bernstein , Sudeb Bhattacharya , Mary Bishai , Thomas Blum , S. Alex Bogacz , Stephen J. Brice , Joachim Brod , Alan Bross , Michael Buchoff , Thomas W. Burgess , Marcela Carena , Luis A. Castellanos , Subhasis Chattopadhyay , Mu-Chun Chen , Daniel Cherdack , Norman H. Christ , Tim Chupp , Vincenzo Cirigliano , Pilar Coloma , Christopher E. Coppola , Ramanath Cowsik , J. Allen Crabtree , André de Gouvêa , Jean-Pierre Delahaye , Dmitri Denisov , Patrick deNiverville , Ranjan Dharmapalan , Markus Diefenthaler , Alexander Dolgov , Georgi Dvali , Estia Eichten , Jürgen Engelfried , Phillip D. Ferguson , Tony Gabriel , Avraham Gal , Franz Gallmeier , Kenneth S. Ganezer , Susan Gardner , Douglas Glenzinski , Stephen Godfrey , Elena S. Golubeva , Stefania Gori , Van B. Graves , Geoffrey Greene , Cory L. Griffard , Ulrich Haisch , Thomas Handler , Brandon Hartfiel , Athanasios Hatzikoutelis , Ayman Hawari , Lawrence Heilbronn , James E. Hill , Patrick Huber , David E. Jaffe , Xiaodong Jiang , Christian Johnson , Yuri Kamyshkov , Daniel M. Kaplan , Boris Kerbikov , Brendan Kiburg , Harold G. Kirk , Andreas Klein , Kyle Knoepfel , Boris Kopeliovich , Vladimir Kopeliovich , Joachim Kopp , Wolfgang Korsch , Graham Kribs , Ronald Lipton , Chen-Yu Liu , Wolfgang Lorenzon , Zheng-Tian Lu , Naomi C. R. Makins , David McKeen , Geoffrey Mills , Michael Mocko , Rabindra Mohapatra , Nikolai V. Mokhov , Guenter Muhrer , Pieter Mumm , David Neuffer , Lev Okun , Mark A. Palmer , Robert Palmer , Robert W. Pattie , David G. Phillips , Kevin Pitts , Maxim Pospelov , Vitaly S. Pronskikh , Chris Quigg , Erik Ramberg , Amlan Ray , Paul E. Reimer , David G. Richards , Adam Ritz , Amit Roy , Arthur Ruggles , Robert Ryne , Utpal Sarkar , Andy Saunders , Yannis K. Semertzidis , Anatoly Serebrov , Hirohiko Shimizu , Robert Shrock , Arindam K. Sikdar , Pavel V. Snopok , William M. Snow , Aria Soha , Stefan Spanier , Sergei Striganov , Zhaowen Tang , Lawrence Townsend , Jon Urheim , Arkady Vainshtein , Richard Van de Water , Ruth S. Van de Water , Richard J. Van Kooten , Bernard Wehring , William C. Wester , Lisa Whitehead , Robert J. Wilson , Elizabeth Worcester , Albert R. Young , Geralyn Zeller

The nuSTORM facility has been designed to deliver beams of electron neutrinos and muon neutrinos (and their anti-particles) from the decay of a stored muon beam with a central momentum of 3.8 GeV/c and a momentum acceptance of 10%. The…

Accelerator Physics · Physics 2017-03-20 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 , P. Coloma , L. Coney , A. Dobbs , J. Dobson , A. Donini , P. Dornan , M. Dracos , F. Dufour , R. Edgecock , J. Evans , M. Geelhoed , M. A. George , T. Ghosh , J. J. Gomez-Cadenas , A. de Gouvea , A. Haesler , G. Hanson , P. F. Harrison , M. Hartz , P. Hernandez , J. A. Hernando Morata , P. Hodgson , P. Huber , A. Izmaylov , Y. Karadzhov , T. Kobilarcik , J. Kopp , L. Kormos , A. Korzenev , Y. Kuno , A. Kurup , P. Kyberd , J. B. Lagrange , A. Laing , A. Liu , J. M. Link , K. Long , K. Mahn , C. Mariani , C. Martin , J. Martin , N. McCauley , K. T. McDonald , 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 , T. Sen , E. Scantamburlo , J. K. Sedgbeer , D. R. Smith , P. J. Smith , J. T. Sobczyk , L. Soby , F. J. P. Soler , S. Soldner-Rembold , M. Sorel , P. Snopok , P. Stamoulis , L. Stanco , S. Striganov , H. A. Tanaka , I. J. Taylor , C. Touramanis , C. D. Tunnell , Y. Uchida , N. Vassilopoulos , M. O. Wascko , A. Weber , M. J. Wilking , E. Wildner , W. Winter , U. K. Yang

With the planned turn-on of the PIP-II 800 MeV superconducting proton linac, Fermilab will potentially become the world's best laboratory at which to carry out fundamental muon measurements, sensitive searches for symmetry violation, and…

We explore the feasibility of a next-generation Mu2e experiment that uses Project-X beams to achieve a sensitivity approximately a factor ten better than the currently planned Mu2e facility.

A superconducting RF accelerator test facility is being constructed at Fermilab. The existing New Muon Lab (NML) building is being converted for this facility. The accelerator will consist of an electron gun, injector, beam acceleration…

Fermilab operates the world's most intense source of antiprotons. Recently various experiments have been proposed that can use those antiprotons either parasitically during Tevatron Collider running or after the Tevatron Collider finishes…

High Energy Physics - Experiment · Physics 2015-05-13 Daniel M. Kaplan

The Long Baseline Neutrino Experiment (LBNE) will utilize a neutrino beamline facility located at Fermilab to carry out a compelling research program in neutrino physics. The facility will aim a beam of neutrinos toward a detector placed at…

Accelerator Physics · Physics 2011-12-06 Vaia Papadimitriou

In Fermilab's neutrino facilities such as the Neutrinos at the Main Injector (NuMI) and the upcoming Long Baseline Neutrino Facility (LBNF), a proton beam strikes high-power target, producing positively and negatively charged pions and…

Accelerator Physics · Physics 2024-01-24 D. A. Wickremasinghe , S. Ganguly , K. Yonehara , R. Zwaska , P. Snopok , Y. Yu

A muon collider would be a powerful tool for exploring the energy-frontier with leptons, and would complement the studies now under way at the LHC. Such a device would offer several important benefits. Muons, like electrons, are point…

Accelerator Physics · Physics 2011-09-15 Michael S. Zisman

The Long Baseline Neutrino Experiment (LBNE) will utilize a neutrino beamline facility located at Fermilab. The facility is designed to aim a beam of neutrinos toward a detector placed in South Dakota. The neutrinos are produced in a…

The Neutrinos at the Main Injector (NuMI) facility at Fermilab began operations in late 2004. NuMI will deliver an intense muon neutrino beam of variable energy (2-20 GeV). Several aspects of the design and results from runs of the MINOS…

High Energy Physics - Experiment · Physics 2009-11-13 Sacha E. Kopp

The Neutrinos at the Main Injector (NuMI) facility at Fermilab began operations in late 2004. NuMI will deliver an intense muon neutrino beam of variable energy (2-20 GeV) directed into the Earth at 58 mrad for short (~1km) and long…

Accelerator Physics · Physics 2007-05-23 Sacha E. Kopp

We propose a new high-resolution neutrino experiment within a dipole magnetic field, HiResM$\nu$. This experiment will run along with long-baseline neutrino oscillation experiments (LBL$\nu$) such as NO$\nu$A, a large-cavity detector at…

High Energy Physics - Experiment · Physics 2009-04-14 S. R. Mishra , R. Petti , C. Rosenfeld