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A Short-Baseline Neutrino (SBN) physics program of three LAr-TPC detectors located along the Booster Neutrino Beam (BNB) at Fermilab is presented. This new SBN Program will deliver a rich and compelling physics opportunity, including the…

Instrumentation and Detectors · Physics 2023-02-17 R. Acciarri , C. Adams , R. An , C. Andreopoulos , A. M. Ankowski , M. Antonello , J. Asaadi , W. Badgett , L. Bagby , B. Baibussinov , B. Baller , G. Barr , N. Barros , M. Bass , V. Bellini , P. Benetti , S. Bertolucci , K. Biery , H. Bilokon , M. Bishai , A. Bitadze , A. Blake , F. Boffelli , T. Bolton , M. Bonesini , J. Bremer , S. J. Brice , C. Bromberg , L. Bugel , E. Calligarich , L. Camilleri , D. Caratelli , B. Carls , F. Cavanna , S. Centro , H. Chen , C. Chi , E. Church , D. Cianci , A. G. Cocco , G. H. Collin , J. M. Conrad , M. Convery , G. De Geronimo , A. Dermenev , R. Dharmapalan , S. Dixon , Z. Djurcic , S. Dytmam , B. Eberly , A. Ereditato , J. Esquivel , J. Evans , A. Falcone , C. Farnese , A. Fava , A. Ferrari , B. T. Fleming , W. M. Foreman , J. Freestone , T. Gamble , G. Garvey , V. Genty , M. Geynisman , D. Gibin , S. Gninenko , D. Göldi , S. Gollapinni , N. Golubev , M. Graham , E. Gramellini , H. Greenlee , R. Grosso , R. Guenette , A. Guglielmi , A. Hackenburg , R. Hänni , O. Hen , V Hewes , J. Ho , G. Horton-Smith , J. Howell , A. Ivashkin , C. James , C. M. Jen , R. A. Johnson , B. J. P. Jones , J. Joshi , H. Jostlein , D. Kaleko , L. N. Kalousis , G. Karagiorgi , W. Ketchum , B. Kirby , M. Kirby , M. Kirsanov , J. Kisiel , J. Klein , J. Klinger , T. Kobilarcik , U. Kose , I. Kreslo , V. A. Kudryavtsev , Y. Li , B. Littlejohn , D. Lissauer , P. Livesly , S. Lockwitz , W. C. Louis , M. Lüthi , B. Lundberg , F. Mammoliti , G. Mannocchi , A. Marchionni , C. Mariani , J. Marshall , K. Mavrokoridis , N. McCauley , N. McConkey , K. McDonald , V. Meddage , A. Menegolli , G. Meng , I. Mercer , T. Miao , T. Miceli , G. B. Mills , D. Mladenov , C. Montanari , D. Montanari , J. Moon , M. Mooney , C. Moore , Z. Moss , M. H. Moulai , S. Mufson , R. Murrells , D. Naples , M. Nessi , M. Nicoletto , P. Nienaber , B. Norris , F. Noto , J. Nowak , S. Pal , O. Palamara , V. Paolone , V. Papavassiliou , S. Pate , J. Pater , Z. Pavlovic , J. Perkin , P. Picchi , F. Pietropaolo , P. Płoński , S. Pordes , R. Potenza , G. Pulliam , X. Qian , L. Qiuguang , J. L. Raaf , V. Radeka , R. Rameika , A. Rappoldi , G. L. Raselli , P. N. Ratoff , B. Rebel , M. Richardson , L. Rochester , M. Rossella , C. Rubbia , C. Rudolf von Rohr , B. Russell , P. Sala , A. Scaramelli , D. W. Schmitz , A. Schukraft , W. Seligman , M. H. Shaevitz , B. Sippach , E. Snider , J. Sobczyk , M. Soderberg , S. Söldner-Rembold , M. Spanu , J. Spitz , N. Spooner , D. Stefan , J. St. John , T. Strauss , R. Sulej , C. M. Sutera , A. M. Szelc , N. Tagg , C. E. Taylor , K. Terao , M. Thiesse , L. Thompson , M. Thomson , C. Thorn , M. Torti , F. Tortorici , M. Toups , C. Touramanis , Y. Tsai , T. Usher , R. Van de Water , F. Varanini , S. Ventura , C. Vignoli , T. Wachala , M. Weber , D. Whittington , P. Wilson , S. Wolbers , T. Wongjirad , K. Woodruff , M. Xu , T. Yang , B. Yu , A. Zani , G. P. Zeller , J. Zennamo , C. Zhang

The Muon Campus at Fermilab provides world class accelerator infrastructure supporting the next generation intensity frontier experiments. The anti-proton source from the Tevatron era was converted to the present day Muon Campus at the end…

Accelerator Physics · Physics 2022-08-08 S. Ganguly

The Minos+ experiment is an extension of the Minos experiment at a higher energy and more intense neutrino beam, with the data collection having begun in the fall of 2013. The neutrino beam is provided by the Neutrinos from the Main…

Instrumentation and Detectors · Physics 2016-11-17 William Badgett , Steve R. Hahn , Donatella Torretta , Jerry Meier , Jeffrey Gunderson , Denise Osterholm , David Saranen

Programmable integrated photonics (PIP) has emerged as a powerful on-chip platform for optical signal processing and computing, enabling the implementation of reconfigurable N$\times$N unitary matrix transformations through meshes of…

The current and future need for high-energy neutrons has been a subject of increasing discussion and concern. Immediate applications for such an intense neutron source include medical isotope production, high-energy physics (HEP) research,…

Accelerator Physics · Physics 2023-03-13 Lance L Snead , Daniel Winklehner , Dennis Whyte , Steve Zinkle , Zach Hartwig , David Sprouster

The Fermilab Tevatron will be the world's highest energy hadron collider until the LHC is commissioned, it has the world's highest energy fixed target beams, and Fermilab will be the leading high energy physics laboratory in the US for the…

High Energy Physics - Experiment · Physics 2007-05-23 D. Amidei , A. Baden , G. Foster , G. Jackson , T. Kamon , J. Lopez , P. McIntyre , J. Strait , J. White

A new beam dump has been designed, built, installed and operated to withstand the future proton beam extracted from the Proton Synchrotron Booster (PSB) in the framework of the LHC Injector Upgrade (LIU) Project at CERN, consisting of up to…

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…

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

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 difference between the rf voltage seen by the beam and the accelerating voltage required to match the rate of change of the Booster magnetic field is used to estimate the energy loss per beam turn. Because the rf voltage (RFSUM) and the…

Accelerator Physics · Physics 2007-05-23 Xi Yang , C. Ankenbrandt , J. Norem

Artificial neural networks are efficient computing platforms inspired by the brain. Such platforms can tackle a vast area of real-life tasks ranging from image processing to language translation. Silicon photonic integrated chips (PICs), by…

Emerging Technologies · Computer Science 2022-10-19 George Sarantoglou , Adonis Bogris , Charis Mesaritakis , Sergios Theodoridis

The new g-2 experiment at Fermilab aims to measure the muon anomalous magnetic moment by a fourfold improvement in precision compared to the BNL experiment. Achieving this goal requires the delivery of highly polarized 3.094 GeV/c muons…

The intensity of charged particle beams at Fermilab must be kept within pre-determined safety and operational envelopes in part by assuring all beam within a few percent has been transported from any source to destination. Beam intensity…

Accelerator Physics · Physics 2012-09-25 J. Crisp , B. Fellenz , J. Fitzgerald , D. Heikkinen , M. A. Ibrahim

We have conducted tests at the Fermilab Booster of ionization chambers to be used as monitors of the NuMI neutrino beamline. The chambers were exposed to proton fluxes of up to 10$^{12}$ particles/cm$^2$/1.56$\mu$s. We studied space charge…

Efficient transport of high-current negative ion beams is critical for accurate plasma potential diagnostics using heavy-ion beam probe (HIBP) systems in magnetically confined fusion plasmas. However, strong space-charge effects often…

Plasma Physics · Physics 2025-09-23 M. Nishiura , K. Nakamura , K. Ueda , A. Shimizu , H. Takubo , M. Kanda , T. Ido , M. Okamura

"LUE200" - 200 MeV electron linac is being created at JINR as a driver of the pulsed neutron source "IREN" [1]. The special full-scale facilities for testing the main systems of LUE-200 (FSTF) are used at JINR, BINP, MEPhI and YerPhI [2].…

Accelerator Physics · Physics 2009-10-05 S. N. Dolya , W. I. Furman , V. V. Kobets , E. M. Laziev , Yu. A. Metelkin , V. A. Shvets , A. P. Soumbaev

For NOvA and future experiments requiring high intensity proton beams, Fermilab is in the process of upgrading the existing accelerator complex for increased proton production. One such improvement is to reduce the Main Injector cycle time,…

Accelerator Physics · Physics 2014-09-22 R. Madrak , V. Kashikhin , A. Makarov , D. Wildman

Starting this summer, Fermilab will host a key experiment dedicated to the search for signals of new physics: The Fermilab Muon g-2 Experiment. Its aim is to precisely measure the anomalous magnetic moment of the muon. In full operation, in…

The Muon g-2 experiment at Fermilab, with the aim to measure the muon anomalous magnetic moment to an unprecedented level of 140~ppb, has started beam and detector commissioning in Summer 2017. To deal with incoming data projected to be…

Instrumentation and Detectors · Physics 2019-08-14 Kim Siang Khaw