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Related papers: FLARE, Fermilab Liquid Argon Experiments

200 papers

The planned neutrino program at Fermilab requires large proton beam intensities in excess of 2 MW. Measuring the transverse profiles of these high intensity beams is challenging and often depends on non-invasive techniques. One such…

Accelerator Physics · Physics 2015-11-09 R. Thurman-Keup , M. Alvarez , J. Fitzgerald , C. Lundberg , P. Prieto , M. Roberts , J. Zagel , W. Blokland

This paper describes the hardware and operations of the Neutrinos at the Main Injector (NuMI) beam at Fermilab. It elaborates on the design considerations for the beam as a whole and for individual elements. The most important design…

Accelerator Physics · Physics 2015-12-09 P. Adamson , K. Anderson , M. Andrews , R. Andrews , I. Anghel , D. Augustine , A. Aurisano , S. Avvakumov , D. S. Ayres , B. Baller , B. Barish , G. Barr , W. L. Barrett , R. H. Bernstein , J. Biggs , M. Bishai , A. Blake , V. Bocean , G. J. Bock , D. J. Boehnlein , D. Bogert , K. Bourkland , S. V. Cao , C. M. Castromonte , S. Childress , B. C. Choudhary , J. A. B. Coelho , J. H. Cobb , L. Corwin , D. Crane , J. P. Cravens , D. Cronin-Hennessy , R. J. Ducar , J. K. de Jong , A. V. Devan , N. E. Devenish , M. V. Diwan , A. R. Erwin , C. O. Escobar , J. J. Evans , E. Falk , G. J. Feldman , T. H. Fields , R. Ford , M. V. Frohne , H. R. Gallagher , V. Garkusha , R. A. Gomes , M. C. Goodman , P. Gouffon , N. Graf , R. Gran , N. Grossman , K. Grzelak , A. Habig , S. R. Hahn , D. Harding , D. Harris , P. G. Harris , J. Hartnell , R. Hatcher , S. Hays , K. Heller , A. Holin , J. Huang , J. Hylen , A. Ibrahim , D. Indurthy , G. M. Irwin , Z. Isvan , D. E. Jaffe , C. James , D. Jensen , J. Johnstone , T. Kafka , S. M. S. Kasahara , G. Koizumi , S. Kopp , M. Kordosky , A. Kreymer , K. Lang , C. Laughton , G. Lefeuvre , J. Ling , P. J. Litchfield , L. Loiacono , P. Lucas , W. A. Mann , A. Marchionni , M. L. Marshak , N. Mayer , C. McGivern , M. M. Medeiros , R. Mehdiyev , J. R. Meier , M. D. Messier , D. G. Michael , R. H. Milburn , J. L. Miller , W. H. Miller , S. R. Mishra , S. Moed Sher , C. D. Moore , J. Morfin , L. Mualem , S. Mufson , S. Murgia , M. Murtagh , J. Musser , D. Naples , J. K. Nelson , H. B. Newman , R. J. Nichol , J. A. Nowak , J. O Connor , W. P. Oliver , M. Olsen , M. Orchanian , S. Osprey , R. B. Pahlka , J. Paley , A. Para , R. B. Patterson , T. Patzak , Z. Pavlovic , G. Pawloski , A. Perch , E. A. Peterson , D. A. Petyt , M. M. Pfutzner , S. Phan-Budd , R. K. Plunkett , N. Poonthottathil , P. Prieto , D. Pushka , X. Qiu , A. Radovic , R. A. Rameika , J. Ratchford , B. Rebel , R. Reilly , C. Rosenfeld , H. A. Rubin , K. Ruddick , M. C. Sanchez , N. Saoulidou , L. Sauer , J. Schneps , D. Schoo , A. Schreckenberger , P. Schreiner , P. Shanahan , R. Sharma , W. Smart , C. Smith , A. Sousa , A. Stefanik , N. Tagg , R. L. Talaga , G. Tassotto , J. Thomas , J. Thompson , M. A. Thomson , X. Tian , A. Timmons , D. Tinsley , S. C. Tognini , R. Toner , D. Torretta , I. Trostin , G. Tzanakos , J. Urheim , P. Vahle , K. Vaziri , E. Villegas , B. Viren , G. Vogel , R. C. Webber , A. Weber , R. C. Webb , A. Wehmann , C. White , L. Whitehead , L. H. Whitehead , S. G. Wojcicki , M. L. Wong-Squires , T. Yang , F. X. Yumiceva , V. Zarucheisky , R. Zwaska

The Deep Underground Neutrino Experiment (DUNE) is a long-baseline neutrino experiment that will precisely measure neutrino oscillation parameters, observe astrophysical neutrinos, and search for processes beyond the Standard Model such as…

High Energy Physics - Experiment · Physics 2024-10-14 Sergio Manthey Corchado

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…

Experiments with low-energy antiprotons are currently performed at the Antiproton Decelerator of CERN. The main experiments deal with the spectroscopy of antiprotonic helium, an exotic three-body system, and the formation and spectroscopy…

High Energy Physics - Experiment · Physics 2010-03-09 E. Widmann

We discuss the possibility of new generation neutrino and astroparticle physics experiments exploiting the liquid Argon Time Projection Chamber (LAr TPC) technique, following a graded strategy that envisions applications with increasing…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Ereditato , A. Rubbia

The Deep Underground Neutrino Experiment (DUNE) Far Detector (FD) will be formed by four 10-kton Liquid Argon (LAr) Time Projection Chambers (TPC) using both single and dual-phase technology. The dual-phase technology foreseen the charge…

Instrumentation and Detectors · Physics 2019-11-19 Chiara Lastoria

Measurements and calculations of the air activation at a high-energy proton accelerator are described. The quantity of radionuclides released outdoors depends on operation scenarios including details of the air exchange inside the facility.…

Accelerator Physics · Physics 2018-03-14 I. L. Rakhno , J. Hylen , P. Kasper , N. V. Mokhov , M. Quinn , S. I. Striganov , K. Vaziri

Part-3 of "Project X: Accelerator Reference Design, Physics Opportunities, Broader Impacts". The proposed Project X proton accelerator at Fermilab, with multi-MW beam power and highly versatile beam formatting, will be a unique world-class…

MicroBooNE is a neutrino experiment that utilizes a liquid argon time projection chamber (LArTPC) located on-axis in the Booster Neutrino Beam (BNB) at Fermilab. One of the experiment's main goals is to search for excess low-energy…

High Energy Physics - Experiment · Physics 2020-12-16 David Caratelli

A staged approach towards muon based facilities for Intensity and Energy Frontier science, building upon existing and proposed facilities at Fermilab, is presented. At each stage, a facility exploring new physics also provides an R&D…

Several different experiments have hinted to the existence of "anomalies" in the neutrino sector, implying the possible presence of additional sterile neutrinos or of other options. A definitive experimental search, capable to clarify…

High Energy Physics - Phenomenology · Physics 2013-04-09 Carlo Rubbia , Alberto Guglielmi , Francesco Pietropaolo , Paola Sala

The Deep Underground Neutrino Experiment (DUNE) will be the first mega-science program on the US soil and will shade light on some of the open questions in neutrino physics. The experiment foresees the realization of an intense neutrino…

Instrumentation and Detectors · Physics 2026-02-17 H. V. Souza

For the future neutrino oscillation experiment DUNE, liquid argon time projections chambers with a fiducial mass of 10 kton each are foreseen. The dual phase concept is one of the two implementations considered, wherein electrons produced…

Instrumentation and Detectors · Physics 2019-05-22 T. Lux

We discuss the possibility of new generation neutrino and astroparticle physics experiments exploiting a superconducting magnetized liquid Argon Time Projection Chamber (LAr TPC). The possibility to complement the features of the LAr TPC…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Ereditato , A. Rubbia

The D0 experiment was designed in the mid 1980s and ran at the Fermilab pp collider from 1992 through 2011. I describe the uranium-liquid argon calorimeter and its readout electronic which was upgraded in the late 1990s to handle the higher…

Instrumentation and Detectors · Physics 2014-03-19 Dean Schamberger

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

The Argon Dark Matter (ArDM) experiment consists of a liquid argon (LAr) time projection chamber (TPC) sensitive to nuclear recoils resulting from scattering of hypothetical Weakly Interacting Massive Particles (WIMPs) on argon targets.…

The recent discovery that neutrinos have masses opens a wide new field of experimentation. Accelerator-made neutrinos are essential in this program. Ideas for future facilities include high intensity muon neutrino beams from pion decay…

High Energy Physics - Phenomenology · Physics 2016-09-06 A. Blondel , A. Cervera-Villanueva , A. Donini , P. Huber , M. Mezzetto , P. Strolin

The Short Baseline Near Detector (SBND) is a 112 ton active mass liquid argon time projection chamber (LArTPC) that will begin operations in the Booster Neutrino Beamline at Fermilab in 2020. Its main physics goals include high-statistics…

Instrumentation and Detectors · Physics 2019-10-21 Georgia Karagiorgi