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The MicroBooNE experiment is an upcoming liquid argon TPC experiment which will pursue a program of short baseline neutrino physics in the Fermilab Booster Neutrino Beam, starting in early 2014. I give a description of the experiment and…

Instrumentation and Detectors · Physics 2011-10-13 Benjamin J P Jones

Two next generation muon $g-2$ experiments at Fermilab in the US and at J-PARC in Japan have been designed to reach a four times better precision from 0.54 ppm to 0.14 ppm and the challenge for the theory side is to keep up in precision as…

High Energy Physics - Phenomenology · Physics 2018-08-01 Fred Jegerlehner

In this document, technical details of the upgrade plan of the J-PARC neutrino beamline for the extension of the T2K experiment are described. T2K has proposed to accumulate data corresponding to $2\times{}10^{22}$ protons-on-target in the…

Instrumentation and Detectors · Physics 2019-08-15 K. Abe , H. Aihara , A. Ajmi , C. Alt , C. Andreopoulos , M. Antonova , S. Aoki , Y. Asada , Y. Ashida , A. Atherton , E. Atkin , S. Ban , F. C. T. Barbato , M. Barbi , G. J. Barker , G. Barr , M. Batkiewicz , A. Beloshapkin , V. Berardi , L. Berns , S. Bhadra , J. Bian , S. Bienstock , A. Blondel , S. Bolognesi , J. Borg , B. Bourguille , S. B. Boyd , D. Brailsford , A. Bravar , S. Bron , C. Bronner , M. Buizza Avanzini , N. F. Calabria , J. Calcutt , R. G. Calland , D. Calvet , T. Campbell , S. Cao , S. L. Cartwright , M. G. Catanesi , A. Cervera , A. Chappell , D. Cherdack , N. Chikuma , G. Christodoulou , M. Cicerchia , A. Clifton , G. Cogo , J. Coleman , G. Collazuol , D. Coplowe , A. Cudd , A. Dabrowska , A. Delbart , A. De Roeck , G. De Rosa , T. Dealtry , A. Dell'acqua , P. F. Denner , S. R. Dennis , C. Densham , D. Dewhurst , F. Di Lodovico , S. Dolan , N. Dokania , D. Doqua , O. Drapier , K. E. Duffy , J. Dumarchez , P. J. Dunne , M. Dziewiecki , L. Eklund , S. Emery-Schrenk , S. Fedotov , P. Fernandez , T. Feusels , A. J. Finch , G. A. Fiorentini , G. Fiorillo , M. Fitton , M. Friend , Y. Fujii , R. Fujita , D. Fukuda , R. Fukuda , Y. Fukuda , K. Fusshoeller , A. Gendotti , C. Giganti , F. Gizzarelli , M. Gonin , A. Gorin , F. Gramegna , M. Guigue , D. R. Hadley , J. T. Haigh , S. -P. Hallsjö , P. Hamacher-Baumann , D. Hansen , J. Harada , M. Hartz , T. Hasegawa , N. C. Hastings , Y. Hayato , A. Hiramoto , M. Hogan , J. Holeczek , F. Iacob , A. K. Ichikawa , M. Ikeda , J. Imber , T. Ishida , T. Ishii , T. Ishii , M. Ishitsuka , E. Iwai , K. Iwamoto , A. Izmaylov , B. Jamieson , M. Jiang , S. Johnson , P. Jonsson , C. K. Jung , M. Kabirnezhad , A. C. Kaboth , T. Kajita , H. Kakuno , J. Kameda , S. Kasetti , Y. Kataoka , T. Katori , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , H. Kim , S. King , J. Kisiel , A. Knight , A. Knox , T. Kobayashi , L. Koch , A. Konaka , L. L. Kormos , A. Korzenev , Y. Koshio , K. Kowalik , W. Kropp , Y. Kudenko , S. Kuribayashi , R. Kurjata , T. Kutter , M. Kuze , L. Labarga , J. Lagoda , I. Lamont , M. Lamoureux , D. Last , M. Laveder , M. Lawe , T. Lindner , Z. J. Liptak , R. P. Litchfield , S. Liu , K. R. Long , A. Longhin , J. P. Lopez , L. Ludovici , X. Lu , T. Lux , L. Magaletti , L. Magro , K. Mahn , M. Malek , S. Manly , T. Marchi , L. Maret , A. D. Marino , J. F. Martin , S. Martynenko , T. Maruyama , T. Matsubara , K. Matsushita , V. Matveev , C. Mauger , K. Mavrokoridis , E. Mazzucato , M. McCarthy , N. McCauley , K. S. McFarland , C. McGrew , A. Mefodiev , C. Metelko , M. Mezzetto , P. Mijakowski , J. Mijakowski , A. Minamino , O. Mineev , S. Mine , A. Missert , M. Miura , L. Molina Bueno , S. Moriyama , J. Morrison , Th. A. Mueller , S. Murphy , Y. Nagai , T. Nakadaira , M. Nakahata , Y. Nakajima , A. Nakamura , K. G. Nakamura , K. Nakamura , S. Nakayama , T. Nakaya , K. Nakayoshi , C. Nantais , T. V. Ngoc , K. Nishikawa , Y. Nishimura , T. Nonnenmacher , F. Nova , P. Novella , J. Nowak , J. C. Nugent , H. M. O'Keeffe , T. Odagawa , R. Ohta , K. Okamoto , K. Okumura , T. Okusawa , T. Ovsyannikova , R. A. Owen , Y. Oyama , V. Palladino , V. Paolone , M. Pari , W. Parker , S. Parsa , J. Pasternak , C. Pastore , M. Pavin , D. Payne , J. D. Perkin , L. Pickard , L. Pickering , E. S. Pinzon Guerra , B. Popov , M. Posiadala-Zezula , J. -M. Poutissou , R. Poutissou , J. Pozimski , P. Przewlocki , H. Przybilsk , B. Quilain , T. Radermacher , E. Radicioni , B. Radics , P. N. Ratoff , E. Reinherz-Aronis , C. Riccio , P. Rojas , E. Rondio , B. Rossi , S. Roth , A. Rubbia , A. C. Ruggeri , C. A. Ruggles , A. Rychter , K. Sakashita , F. Sánchez , C. M. Schloesser , K. Scholberg , J. Schwehr , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , D. Sgalaberna , A. Shaikina , R. Shah , A. Shaikhiev , F. Shaker , D. Shaw , M. Shiozawa , T. Shirahige , W. Shorrock , A. Smirnov , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , L. Southwell , R. Spina , J. Steinmann , T. Stewart , P. Stowell , S. Suvorov , A. Suzuki , S. Y. Suzuki , Y. Suzuki , J. Swierblewski , M. Szeptycka , S. Szoldos , A. Sztuc , R. Tacik , M. Tada , M. Tajima , A. Takeda , Y. Takeuchi , H. K. Tanaka , H. A. Tanaka , L. F. Thompson , W. Toki , T. Tomura , C. Touramanis , K. Tsui , T. Tsukamoto , M. Tzanov , M. A. Uchida , Y. Uchida , M. Vagins , N. H. Van , G. Vasseur , T. Viant , C. Vilela , T. Wachala , C. W. Walter , Y. Wang , D. Wark , M. O. Wascko , A. Weber , R. Wendell , R. J. Wilkes , M. J. Wilking , J. R. Wilson , R. J. Wilson , K. Wood , C. Wret , Y. Yamada , K. Yamamoto , C. Yanagisawa , G. Yang , T. Yano , K. Yasutome , S. Yen , N. Yershov , M. Yokoyama , T. Yoshida , T. Yuan , M. Yu , A. Zalewska , J. Zalipska , L. Zambelli , K. Zaremba , M. Ziembicki , E. D. Zimmerman , M. Zito , E. Hamada , N. Higashi , E. Hirose , Y. Igarashi , M. Iida , M. Iio , M. Ikeno , N. Kimura , N. Kurosawa , Y. Makida , T. Nakamoto , T. Ogitsu , H. Ohhata , R. Okada , T. Okamura , M. Onaka , K. Sasaki , S. Shimazaki , M. Shoji , M. Sugano , K. Tanaka , M. Tanaka , A. Terashima , T. Tomaru , T. Uchida , M. Yoshida

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 Facility (LBNF) will utilize a beamline located at Fermilab to provide and aim a neutrino beam of sufficient intensity and appropriate energy range toward the Deep Underground Neutrino Experiment (DUNE) detectors,…

A portion of the remnant Tevatron program infrastructure at Fermilab is being reconfigured to be used for the generation and delivery of proton and muon beams for new high-precision particle physics experiments. With the 8 GeV Booster as…

Accelerator Physics · Physics 2016-12-23 J. A. Johnstone , M. J. Syphers

To maximize the physics potential of future neutrino oscillation experiments, it is proposed to build a 15-MW `proton driver' consisitng solely of a 3-GeV proton injector linac (PI) and a 17-GeV superconducting ILC-type linac (SCL). The…

Accelerator Physics · Physics 2019-03-25 Radoje Belusevic

In order to develop an RF cavity that is applicable for a muon beam cooling channel, a new facility, called Mucool Test Area (MTA) has been built at Fermilab. MTA is a unique facility whose purpose is to test RF cavities in various…

Accelerator Physics · Physics 2019-08-15 Katsuya Yonehara

The CERN accelerator complex prepares protons for the four big experiments at the Interaction Regions of the Large Hadron Collider (LHC) as well as for a number of fixed target experiments, which take beam directly from the LHC injectors.…

Accelerator Physics · Physics 2022-03-18 Hannes Bartosik , Giovanni Rumolo

We have measured cross sections for forward neutron production from a variety of targets using proton beams from the Fermilab Main Injector. Measurements were performed for proton beam momenta of 58 GeV/c, 84 GeV/c, and 120 GeV/c. The cross…

No fast neutron therapy facility has been built with optimized beam quality based on a thorough understanding of the neutron spectrum and its resulting biological effectiveness. A study has been initiated to provide the information…

Accelerator Physics · Physics 2012-07-09 T. K. Kroc

We describe some of the challenges of particle accelerator control, highlight recent advances in neural network techniques, discuss some promising avenues for incorporating neural networks into particle accelerator control systems, and…

Accelerator Physics · Physics 2016-10-21 A. L. Edelen , S. G. Biedron , B. E. Chase , D. Edstrom , S. V. Milton , P. Stabile

Detrimental beam dynamics effects limit performance of high intensity rapid cycling synchrotrons (RCS) such as the 8 GeV proton Fermilab Booster. Here we report the results of comprehensive experimental studies of various beam intensity…

Accelerator Physics · Physics 2021-04-14 Jeff Eldred , Valeri Lebedev , Kiyomi Seiya , Vladimir Shiltsev

Neutrino oscillations provide an unique opportunity to probe physics beyond the Standard Model. Fermilab is constructing two new neutrino beams to provide a decicive test of two of the recent positive indications for neutrino oscillations:…

High Energy Physics - Phenomenology · Physics 2011-04-20 Adam Para

We outline a strategy for next-generation neutrino physics experiments based on beams from accelerators in North America. This strategy is based on the mounting evidence in favor of the large mixing angle solution to solar neutrino problem,…

High Energy Physics - Experiment · Physics 2007-05-23 Kirk T McDonald

MINOS is an accelerator neutrino oscillation experiment at Fermilab. An intense high energy neutrino beam is produced at Fermilab and sent to a near detector on the Fermilab site and also to a 5 kTon far detector 735 km away in the Soudan…

High Energy Physics - Experiment · Physics 2009-05-22 Milind V. Diwan

A new mechanism is suggested for efficient proton acceleration in the GeV energy range; applications to non-conventional high intensity proton drivers and, hence, to low-energy (10-200 MeV) neutrino sources are discussed. In particular we…

High Energy Physics - Phenomenology · Physics 2014-11-17 S. V. Bulanov , T. Esirkepov , P. Migliozzi , F. Pegoraro , T. Tajima , F. Terranova

The Proton Improvement Plan, Stage Two (PIP-II) is a program of upgrades proposed for the Fermilab injection complex, which central part is an 800 MeV, 2 mA CW SRF linac. A prototype of the PIP-II linac front end called PIP-II Injector Test…

Accelerator Physics · Physics 2018-08-28 A. Shemyakin , J. -P. Carneiro , B. Hanna , V. Lebedev , L. Prost , A. Saini , V. Scarpine , V. L. S. Sista , C. Richard

The Mu2e experiment at Fermilab will search for the charged lepton flavour violating process of coherent neutrinoless muon-to-electron conversion in the presence of an aluminum nucleus. The muons are produced by an 8 GeV proton beam from…

Accelerator Physics · Physics 2025-09-29 Z. Liu , J. Williams , A. Makovec , M. Hedges , F. Pellemoine , K. Yonehara , G. Annala , K. Lynch , M. Bloomer , J. Popp , A. Edmonds , J. Miller

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
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