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The PIP-II superconducting RF linac is currently under construction at Fermilab and is expected to be completed by the end of 2028. PIP-II is capable of operating in a continuous-wave mode and can concurrently supply 800 MeV protons to a…

In a dedicated run where protons from the Fermilab Booster were delivered directly to the steel beam dump of the Booster Neutrino Beamline (BNB), the MiniBooNE detector was used to search for the production of sub-GeV dark matter particles…

High Energy Physics - Experiment · Physics 2020-01-29 Alexis A. Aguilar-Arevalo

The MiniBooNE-DM collaboration searched for vector-boson mediated production of dark matter using the Fermilab 8 GeV Booster proton beam in a dedicated run with $1.86 \times 10^{20}$ protons delivered to a steel beam dump. The MiniBooNE…

Short-baseline neutrino (SBN) facilities are optimal for new-physics searches, including the possible production of new particles in and along the neutrino beamline. One such class of models considers states that are created by neutrino…

High Energy Physics - Phenomenology · Physics 2025-07-11 Bhaskar Dutta , Debopam Goswami , Aparajitha Karthikeyan , Kevin J. Kelly

A search for sub-GeV dark matter produced from collisions of the Fermilab 8 GeV Booster protons with a steel beam dump was performed by the MiniBooNE-DM Collaboration using data from $1.86 \times 10^{20}$ protons on target in a dedicated…

Accelerator-based neutrino experiments with high-intensity proton beams and advanced detector technologies provide a powerful and complementary approach to probing physics beyond the Standard Model. The MiniBooNE experiment at Fermilab…

High Energy Physics - Phenomenology · Physics 2026-03-30 Bhaskar Dutta , Debopam Goswami , Aparajitha Karthikeyan , Vishvas Pandey , Zahra Tabrizi , Adrian Thompson , Richard G. Van de Water

The Fermilab Proton Improvement Plan II, or PIP-II, would enable the world's most intense high-energy neutrino beam and would help scientists search for rare particle physics processes. The PIP-II goal is to deliver 1.2 MW of proton beam…

Accelerator Physics · Physics 2022-02-15 Sergei Nagaitsev , Valeri Lebedev

The Fermilab Proton-Improvement-Plan-II (PIP-II) is being implemented in order to support the precision neutrino oscillation measurements at the Deep Underground Neutrino Experiment, the U.S. flagship neutrino experiment. The PIP-II LINAC…

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…

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

We study the sensitivity of the Fermilab Short-Baseline Neutrino (SBN) experiments, MicroBooNE, ICARUS, and SBND, to MeV- to GeV-scale inelastic dark matter interacting through a dark photon mediator. These models provide interesting…

High Energy Physics - Phenomenology · Physics 2021-11-03 Brian Batell , Joshua Berger , Luc Darmé , Claudia Frugiuele

Nearly-sterile neutrinos with masses in the MeV range and below would be produced in the beam of the Short-Baseline Neutrino (SBN) program at Fermilab. In this article, we study the potential for SBN to discover these particles through…

High Energy Physics - Phenomenology · Physics 2017-05-24 Peter Ballett , Silvia Pascoli , Mark Ross-Lonergan

High-intensity neutrino beam facilities may produce a beam of light dark matter when protons strike the target. Searches for such a dark matter beam using its scattering in a nearby detector must overcome the large neutrino background. We…

High Energy Physics - Phenomenology · Physics 2016-05-04 Pilar Coloma , Bogdan A. Dobrescu , Claudia Frugiuele , Roni Harnik

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 study the sensitivity to sub-GeV dark sectors of high energy ($ \geq100$ GeV) proton fixed target experiments such as the Main Injector and the future Long-Baseline Neutrino Facility (LBNF). We focus on off-axis detectors since they have…

High Energy Physics - Phenomenology · Physics 2017-08-02 Claudia Frugiuele

The Fermilab Short-Baseline Neutrino (SBN) experiments, MicroBooNE, ICARUS, and SBND, are expected to have significant sensitivity to light weakly coupled hidden sector particles. Here we study the capability of the SBN experiments to probe…

High Energy Physics - Phenomenology · Physics 2025-10-10 Brian Batell , Joshua Berger , Ahmed Ismail

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,…

Experiments designed to measure neutrino oscillations also provide major opportunities for discovering very weakly coupled states. In order to produce neutrinos, experiments such as LSND collide thousands of Coulombs of protons into fixed…

High Energy Physics - Phenomenology · Physics 2010-12-24 Rouven Essig , Roni Harnik , Jared Kaplan , Natalia Toro

PIP-II is the Fermilab's flagship project for providing powerful, high-intensity proton beams to the laboratory's experiments. The heart of PIP-II is an 800-MeV superconducting linac accelerator. It will be located in a new tunnel with new…

Accelerator Physics · Physics 2018-06-18 L. Lari , F. Cerutti , L. S. Esposito , C. Baffes , S. J. Dixon , N. V. Mokhov , I. Rakhno , I. S. Tropin

The Fermilab proton source is capable of providing 8 GeV protons for both the future long-baseline neutrino program (NuMI), and for a new program of low energy muon experiments. In particular, if the 8 GeV protons are rebunched and then…

Accelerator Physics · Physics 2007-05-23 C. Ankenbrandt , D. Bogert , F. DeJongh , S. Geer , D. McGinnis , D. Neuffer , M. Popovic , E. Prebys
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