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Related papers: Status and Plans for an SRF Accelerator Test Facil…

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In Fermilab we are build and tested several superconducting Single Spoke Resonators (SSR1, \beta=0.22) which can be used for acceleration of low beta ions. Fist two cavities performed very well during cold test in Vertical Test Station at…

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

The S-DALINAC is a 130 MeV superconducting recirculating electron accelerator serving several nuclear and radiation physics experiments as well as driving an infrared free-electron laser. A system of normal conducting rf resonators for…

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

This review paper describes the energy-upgraded CEBAF accelerator. This superconducting linac has achieved 12 GeV beam energy by adding 11 new high-performance cryomodules containing eighty-eight superconducting cavities that have operated…

Accelerator Physics · Physics 2024-09-02 P. A. Adderley , S. Ahmed , T. Allison , R. Bachimanchi , K. Baggett , M. BastaniNejad , B. Bevins , M. Bevins , M. Bickley , R. M. Bodenstein , S. A. Bogacz , M. Bruker , A. Burrill , L. Cardman , J. Creel , Y. -C. Chao , G. Cheng , G. Ciovati , S. Chattopadhyay , J. Clark , W. A. Clemens , G. Croke , E. Daly , G. K. Davis , J. Delayen , S. U. De Silva , R. Dickson , M. Diaz , M. Drury , L. Doolittle , D. Douglas , E. Feldl , J. Fischer , A. Freyberger , V. Ganni , R. L. Geng , C. Ginsburg , J. Gomez , J. Grames , J. Gubeli , J. Guo , F. Hannon , J. Hansknecht , L. Harwood , J. Henry , C. Hernandez-Garcia , S. Higgins , D. Higinbotham , A. S. Hofler , T. Hiatt , J. Hogan , C. Hovater , A. Hutton , C. Jones , K. Jordan , M. Joyce , R. Kazimi , M. Keesee , M. J. Kelley , C. Keppel , A. Kimber , L. King , P. Kjeldsen , P. Kneisel , J. Koval , G. A. Krafft , G. Lahti , T. Larrieu , R. Lauze , C. Leemann , R. Legg , R. Li , F. Lin , D. Machie , J. Mammosser , K. Macha , K. Mahoney , F. Marhauser , B. Mastracci , J. Matalevich , J. McCarter , M. McCaughan , L. Merminga , R. Michaud , V. Morozov , C. Mounts , J. Musson , R. Nelson , W. Oren , R. B. Overton , G. Palacios-Serrano , H. -K. Park , L. Phillips , S. Philip , F. Pilat , T. Plawski , M. Poelker , P. Powers , T. Powers , J. Preble , T. Reilly , R. Rimmer , C. Reece , H. Robertson , Y. Roblin , C. Rode , T. Satogata , D. J. Seidman , A. Seryi , A. Shabalina , I. Shin , R. Slominski , C. Slominski , M. Spata , D. Spell , J. Spradlin , M. Stirbet , M. L. Stutzman , S. Suhring , K. Surles-Law , R. Suleiman , C. Tennant , H. Tian , D. Turner , M. Tiefenback , O. Trofimova , A. -M. Valente , H. Wang , Y. Wang , K. White , C. Whitlatch , T. Whitlatch , M. Wiseman , M. J. Wissman , G. Wu , S. Yang , B. Yunn , S. Zhang , Y. Zhang

The design, construction, and commissioning of a conduction-cooled Nb3Sn demonstration superconducting radio frequency (SRF) electron accelerator at the Institute of Modern Physics of the Chinese Academy of Sciences (IMP, CAS) will be…

PIP-II is an 800 MeV superconducting RF linear accelerator under development at Fermilab. As the new first stage in our accelerator chain, it will deliver high-power beam to multiple experiments simultaneously and thus drive Fermilab's…

Accelerator Physics · Physics 2024-01-30 Dennis J. Nicklaus , Pierrick Hanlet , Charles King , Daniel McArthur , Richard Neswold

Two barrier RF systems were fabricated, tested and installed in the Fermilab Main Injector. Each can provide 8 kV rectangular pulses (the RF barriers) at 90 kHz. When a stationary barrier is combined with a moving barrier, injected beams…

Accelerator Physics · Physics 2010-01-18 W. Chou , D. Capista , J. Griffin , K-Y. Ng , D. Wildman

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…

The CLIC Test Facility (CTF3) is an intermediate step to demonstrate the technical feasibility of the key concepts of the new RF power source for CLIC. CTF3 will use electron beams with an energy range adjustable from 170 MeV (3.5 A) to 380…

Accelerator Physics · Physics 2008-11-26 L. Rinolfi , H. Braun , R. Pittin , F. Zhou , B. Mouton , R. Miller , D. Yeremian

The Advanced Superconducting Test Accelerator (ASTA) facility is currently under construction at Fermilab. With a 1-ms macropulse composed of up to 3000 micropulses and with beam energies projected from 45 to 800 MeV, the need for…

Accelerator Physics · Physics 2014-09-01 A. H. Lumpkin , M. Wendt , J. M. Byrd

The Integrable Optics Test Accelerator (IOTA) is a storage ring for advanced beam physics research currently being built and commissioned at Fermilab. It will operate with protons and electrons using injectors with momenta of 70 and 150…

The Integrable Optics Test Accelerator (IOTA) is proposed for operation at Fermilab. The goal of IOTA is to create practical nonlinear accelerator focusing systems with a large frequency spread and stable particle motion. The IOTA is a 40 m…

Accelerator Physics · Physics 2016-07-04 M. W. McGee , R. Andrews , K. Carlson , J. Leibfritz , L. Nobrega , A. Valishev

A concept for a two-stage injection-locked CW magnetron intended to drive Superconducting Cavities (SC) for intensity-frontier accelerators has been proposed. The concept considers two magnetrons in which the output power differs by 15-20…

The Fermilab Proton Source machines, constituted by Pre-Injector, conventional Linac and Booster synchrotron, at Fermi National Accelerator Laboratory (Fermilab) had have a long history of successful beam operations. Built in late '60s, the…

Accelerator Physics · Physics 2014-09-01 F. G. Garcia , W. Pellico

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…

A semi-empirical method that allows us to predict intensity of generated field emission in superconducting RF cavities is described. Spatial, angular and energy distributions of the generated radiation are calculated with the FISHPACT code.…

Accelerator Physics · Physics 2012-02-09 Camille Ginsburg , Igor Rakhno

SRF cavities for particle acceleration are conventionally operated immersed in a bath of liquid helium at 4.2 K and below. Although this cooling configuration is practically and economically viable for large scientific accelerator…

Accelerator Physics · Physics 2022-07-13 R. C. Dhuley , S. Posen , M. I. Geelhoed , J. C. T. Thangaraj

Project-X is the proposed high intensity proton facility to be built at Fermilab, US. Its Superconducting Linac, to be used at first stage of acceleration, will be operated in continuous wave (CW) mode. The Linac is divided into three…

Accelerator Physics · Physics 2012-02-27 A. Saini , K. Ranjan , N. Solyak , S. Mishra , V. Yakovlev

Fermi National Accelerator Laboratory (FNAL) and Lawrence Berkeley National Laboratory (LBNL) are building a new High Field Vertical Magnet Test Facility (HFVMTF) for testing superconducting cables in high magnetic field. The background…

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