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Fermilab's Superconducting RF Beam Test Facility currently under construction will produce electron beams capable of damaging the acceleration structures and the beam line vacuum chambers in the event of an aberrant accelerator pulse. The…

Accelerator Physics · Physics 2012-10-01 A. Warner , L. Carmichael , M. Church , R. Neswold

Luminosity-driven channeling extraction has been observed for the first time in a 900 GeV study at the Fermilab Tevatron. This experiment, Fermilab E853, demonstrated that useful TeV level beams can be extracted from a superconducting…

As a part of a feasibility study of using the Fermilab Electron Cooler for a low-energy Relativistic Heavy Ion Collider (RHIC) run at Brookhaven National Laboratory (BNL), the cooler operation at 1.6 MeV electron beam energy was tested in a…

Accelerator Physics · Physics 2012-07-26 Lionel Prost , Alexander Shemyakin , Alexei Fedotov , Jorg Kewisch

The beam-profile diagnostics station prototype for the superconducting rf electron linac being constructed at Fermilab at the New Muon Lab has been tested. The station uses intercepting radiation converter screens for the low-power beam…

Accelerator Physics · Physics 2012-08-22 A. Lumpkin , R. Flora , A. S. Johnson , J. Ruan , J. Santucci , V. Scarpine , Y. -E. Sun , R. Thurman-Keup , M. Church , M. Wendt

The Fermilab Linac delivers a variable intensity, 400-MeV beam to the The MuCool Test Area experimental hall via a beam line specifically designed to facilitate measurements of the Linac beam emittance and properties. A 10 m,…

Accelerator Physics · Physics 2013-01-30 F. G. G. Garcia , C. Johnstone , T. Kobilarcik , G. M. Koizumi , C. D. Moore , D. L. Newhart

We report a study of muon neutrino charged-current quasi-elastic events in the segmented scintillator inner tracker of the MINERvA experiment running in the NuMI neutrino beam at Fermilab. The events were selected by requiring a {\mu}^- and…

High Energy Physics - Experiment · Physics 2014-11-25 The MINERvA collaboration , G. A. Fiorentini , D. W. Schmitz , P. A. Rodrigues , L. Aliaga , O. Altinok , B. Baldin , A. Baumbaugh , A. Bodek , D. Boehnlein , S. Boyd , R. Bradford , W. K. Brooks , H. Budd , A. Butkevich , D. A. Martinez Caicedo , C. M. Castromonte , M. E. Christy , H. Chung , J. Chvojka , M. Clark , H. da Motta , D. S. Damiani , I. Danko , M. Datta , M. Day , R. DeMaat , J. Devan , E. Draeger , S. A. Dytman , G. A. Díaz , B. Eberly , D. A. Edmondson , J. Felix , T. Fitzpatrick , L. Fields , A. M. Gago , H. Gallagher , C. A. George , J. A. Gielata , C. Gingu , B. Gobbi , R. Gran , N. Grossman , J. Hanson , D. A. Harris , J. Heaton , A. Higuera , I. J. Howley , K. Hurtado , M. Jerkins , T. Kafka , J. Kaisen , M. O. Kanter , C. E. Keppel , J. Kilmer , M. Kordosky , A. H. Krajeski , S. A. Kulagin , T. Le , H. Lee , A. G. Leister , G. Locke , G. Maggi , E. Maher , S. Manly , W. A. Mann , C. M. Marshall , K. S. McFarland , C. L. McGivern , A. M. McGowan , A. Mislivec , J. G. Morfń , J. Mousseau , D. Naples , J. K. Nelson , G. Niculescu , I. Niculescu , N. Ochoa , C. D. O'Connor , J. Olsen , B. Osmanov , J. Osta , J. L. Palomino , V. Paolone , J. Park , C. E. Patrick , G. N. Perdue , C. Peña , L. Rakotondravohitra , R. D. Ransome , H. Ray , L. Ren , C. Rude , K. E. Sassin , H. Schellman , R. M. Schneider , E. C. Schulte , C. Simon , F. D. Snider , M. C. Snyder , J. T. Sobczyk , C. J. Solano Salinas , N. Tagg , W. Tan , B. G. Tice , G. Tzanakos , J. P. Velásquez , J. Walding , T. Walton , J. Wolcott , B. A. Wolthuis , N. Woodward , G. Zavala , H. B. Zeng , D. Zhang , L. Y. Zhu , B. P. Ziemer

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

This paper describes the design and construction of the MicroBooNE liquid argon time projection chamber and associated systems. MicroBooNE is the first phase of the Short Baseline Neutrino program, located at Fermilab, and will utilize the…

Instrumentation and Detectors · Physics 2023-02-17 MicroBooNE Collaboration , R. Acciarri , C. Adams , R. An , A. Aparicio , S. Aponte , J. Asaadi , M. Auger , N. Ayoub , L. Bagby , B. Baller , R. Barger , G. Barr , M. Bass , F. Bay , K. Biery , M. Bishai , A. Blake , V. Bocean , D. Boehnlein , V. D. Bogert , T. Bolton , L. Bugel , C. Callahan , L. Camilleri , D. Caratelli , B. Carls , R. Castillo Fernandez , F. Cavanna , S. Chappa , H. Chen , K. Chen , C. Y. Chi , C. S. Chiu , E. Church , D. Cianci , G. H. Collin , J. M. Conrad , M. Convery , J. Cornele , P. Cowan , J. I. Crespo-Anadon , G. Crutcher , C. Darve , R. Davis , M. Del Tutto , D. Devitt , S. Duffin , S. Dytman , B. Eberly , A. Ereditato , D. Erickson , L. Escudero Sanchez , J. Esquivel , S. Farooq , J. Farrell , D. Featherston , B. T. Fleming , W. Foreman , A. P. Furmanski , V. Genty , M. Geynisman , D. Goeldi , B. Goff , S. Gollapinni , N. Graf , E. Gramellini , J. Green , A. Greene , H. Greenlee , T. Griffin , R. Grosso , R. Guenette , A. Hackenburg , R. Haenni , P. Hamilton , P. Healey , O. Hen , E. Henderson , V Hewes , C. Hill , K. Hill , L. Himes , J. Ho , G. Horton-Smith , D. Huffman , C. M. Ignarra , C. James , E. James , J. Jan de Vries , W. Jaskierny , C. M. Jen , L. Jiang , B. Johnson , M. Johnson , R. A. Johnson , B. J. P. Jones , J. Joshi , H. Jostlein , D. Kaleko , L. N. Kalousis , G. Karagiorgi , T. Katori , P. Kellogg , W. Ketchum , J. Kilmer , B. King , B. Kirby , M. Kirby , E. Klein , T. Kobilarcik , I. Kreslo , R. Krull , R. Kubinski , G. Lange , F. Lanni , A. Lathrop , A. Laube , W. M. Lee , Y. Li , D. Lissauer , A. Lister , B. R. Littlejohn , S. Lockwitz , D. Lorca , W. C. Louis , G. Lukhanin , M. Luethi , B. Lundberg , X. Luo , G. Mahler , I. Majoros , D. Makowiecki , A. Marchionni , C. Mariani , D. Markley , J. Marshall , D. A. Martinez Caicedo , K. T. McDonald , D. McKee , A. McLean , J. Mead , V. Meddage , T. Miceli , G. B. Mills , W. Miner , J. Moon , M. Mooney , C. D. Moore , Z. Moss , J. Mousseau , R. Murrells , D. Naples , P. Nienaber , B. Norris , N. Norton , J. Nowak , M. OBoyle , T. Olszanowski , O. Palamara , V. Paolone , V. Papavassiliou , S. F. Pate , Z. Pavlovic , R. Pelkey , M. Phipps , S. Pordes , D. Porzio , G. Pulliam , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , R. A Rameika , B. Rebel , R. Rechenmacher , S. Rescia , L. Rochester , C. Rudolf von Rohr , A. Ruga , B. Russell , R. Sanders , W. R. Sands , M. Sarychev , D. W. Schmitz , A. Schukraft , R. Scott , W. Seligman , M. H. Shaevitz , M. Shoun , J. Sinclair , W. Sippach , T. Smidt , A. Smith , E. L. Snider , M. Soderberg , M. Solano-Gonzalez , S. Soldner-Rembold , S. R. Soleti , J. Sondericker , P. Spentzouris , J. Spitz , J. St. John , T. Strauss , K. Sutton , A. M. Szelc , K. Taheri , N. Tagg , K. Tatum , J. Teng , K. Terao , M. Thomson , C. Thorn , J. Tillman , M. Toups , Y. T. Tsai , S. Tufanli , T. Usher , M. Utes , R. G. Van de Water , C. Vendetta , S. Vergani , E. Voirin , J. Voirin , B. Viren , P. Watkins , M. Weber , T. Wester , J. Weston , D. A. Wickremasinghe , S. Wolbers , T. Wongjirad , K. Woodruff , K. C. Wu , T. Yang , B. Yu , G. P. Zeller , J. Zennamo , C. Zhang , M. Zuckerbrot

A fibre detector with multianode PM readout for high rate applications was developed for the HERA-B spectometer to cover the area near the beampipe. Such a detector has to operate at particle rates up to 2*10**4 mm**(-2) s**(-1) and has to…

High Energy Physics - Experiment · Physics 2007-05-23 H. B. Dreis , F. Eisele , M. Hildebrandt , B. Schmidt , A. Sponsel , M. Ziegler

The Booster Neutrino Beamline experiment re-quested a new secondary electron emission multiwire profile monitor installation. The device had to be durable in high radiation conditions and mounted within a large 10-foot airtight steel…

Accelerator Physics · Physics 2024-02-01 R. Prokop

A Monte Carlo simulation has been developed to predict the spatial resolution of silicon pixel detectors. The results discussed in this paper focus on the unit cell geometry of 50 $\mu$m x 400 $\mu$m, as chosen for BTeV. Effects taken into…

High Energy Physics - Experiment · Physics 2009-10-31 Marina Artuso , Jianchun Wang

The MTA beam line has been specifically designed to facilitate measurements of the Fermilab Linac beam emittance and properties utilizing a long, 10m, element-free straight. Linac beam is extracted downstream of the 400-MeV electrostatic…

Accelerator Physics · Physics 2012-09-26 C. Johnstone

A magnetized large-volume liquid scintillator might be used as a tracking detector with charge identification to measure high-energy neutrinos. I consider neutrino oscillations for a beam from a low-energy neutrino factory to such a…

High Energy Physics - Phenomenology · Physics 2009-12-15 Juha Peltoniemi

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

In the context of the evaluation of possibly using the Fermilab Electron Cooler for the proposed low-energy RHIC run at BNL, operating the cooler at 1.6 MeV electron beam energy was tested in a short beam line configuration. The main…

Accelerator Physics · Physics 2012-09-13 L. R. Prost , A. Shemyakin , A. Fedotov , J. Kewisch

A superconducting RF accelerator test facility is currently under construction at Fermilab. The accelerator will consist of an electron gun, 40 MeV injector, beam acceleration section consisting of 3 TTF-type or ILC-type cryomodules, and…

Accelerator Physics · Physics 2012-09-19 M. Church , J. Leibfritz , S. Nagaitsev

Many experimental efforts are striving to provide deep maps of the cosmic microwave background (CMB) to shed light on key questions in modern cosmology. The primary science goal for some of these experiments is to further constrain the…

Instrumentation and Methods for Astrophysics · Physics 2024-08-14 Rustam Balafendiev , Thomas Gascard , Jon E. Gudmundsson

The GERmanium Detector Array, GERDA, searches for neutrinoless double beta decay in Ge-76 using bare high-purity germanium detectors submerged in liquid argon. For the calibration of these detectors gamma emitting sources have to be lowered…

Instrumentation and Detectors · Physics 2013-08-13 Laura Baudis , Alfredo D. Ferella , Francis Froborg , Michal Tarka

For the purpose of withstanding very high radiation doses, silicon pixel sensors with a 3D electrode geometry are being developed. Detectors of this kind are highly interesting for harch radiation environments such as expected in the High…

A large-area and light-weight Gas Electron Multiplier (GEM) detector was built at the University of Virginia as a prototype for the detector R$\&$D program of the future Electron Ion Collider. The prototype has a trapezoidal geometry…

Instrumentation and Detectors · Physics 2025-07-03 Kondo Gnanvo , Xinzhan Bai , Chao Gua , Nilanga Liyanage , Vladimir Nelyubin , Yuxiang Zhao