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High-beta superconducting radiofrequency (SRF) elliptical cavities are being developed for several accelerator projects including Project X, the European XFEL, and the International Linear Collider (ILC). Fermilab has recently established…

Accelerator Physics · Physics 2009-10-23 C. M. Ginsburg

A new test stand dedicated to Superconducting Radiofrequency (SRF) cryomodule testing, CMTS1, has been commissioned and is now in operation at Fermilab. The first device to be cooled down and powered in this facility is the prototype 1.3…

Ir\`{e}ne Joliot-Curie Laboratory (IJCLab) has been leading the development of spoke resonators in multiple international SRF projects, from fundamental R\&D, prototyping, to series production. The European Spallation Source (ESS)…

Accelerator Physics · Physics 2023-06-21 A. Miyazaki , P. Duchesne , D. Ledrean , D. Longuevergne , G. Olry

We demonstrate practical accelerating gradients on a superconducting radiofrequency (SRF) accelerator cavity with cryocooler conduction cooling, a cooling technique that does not involve the complexities of the conventional liquid helium…

Instrumentation and Detectors · Physics 2020-07-09 R. C. Dhuley , S. Posen , M. I. Geelhoed , O. Prokofiev , J. C. T. Thangaraj

PIP-II is a superconducting linac that is in the initial acceleration chain for the Fermilab accelerator complex. The RF system consists of a warm front-end with an RFQ and buncher cavities along with 25 superconducting cryo-modules…

Accelerator Physics · Physics 2025-10-29 P. Varghese , S. Raman , M. Guran , L. Reyes , L. Doolittle , Q. Du , S. Murthy

Commissioning and operation of the first Tesla-style Cryomodule (CM-1) at Fermilab was concluded in recent months. A second Tesla Type III+ module, RFCA002, will be replacing it. CM-1 is the first 8-cavity ILC style cryomodule to be built…

We present a novel hybrid CMOS-MQCA architecture using multi-layer Spintronic devices as computing elements. A feasibility study is presented with 22nm CMOS where new approaches for spin transfer torque induced clocking and read-out scheme…

Emerging Technologies · Computer Science 2012-03-20 Jayita Das , Syed M. Alam , Srinath Rajaram , Sanjukta Bhanja

The higher efficiency of superconducting radio-frequency (SRF) cavities compared to normal-conducting ones enables the development of high-energy continuous-wave linear accelerators (linacs). Recent progress in the development of…

A 5-MeV RFQ designed for a proton current up to 100-mA CW is now under construction as part of the High Intensity Proton Injector project (IPHI). Its computed transmission is greater than 99 %. The main goals of the project are to verify…

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…

At the end of the Large Hadron Collider's Run 2, CERN's Proton Injector Linac 2, commissioned in 1978, delivered its final beam in December 2018. For Run 3, from March 2021, a new H$^{-}$ will take over the role: Linac4. The machine has…

Accelerator Physics · Physics 2019-10-22 Bartosz Bielawski , Philippe Baudrenghien , Robert Borner

The Advanced Superconducting Test Acccelerator (ASTA) 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…

The 75-keV injector and 6.7-MeV RFQ that comprise the first portion of the cw, 100-mA proton linac for the accelerator production of tritium (APT) project have been built and operated. The LEDA RFQ has been extensively tested for pulsed and…

Accelerator Physics · Physics 2012-08-27 H. Vernon Smith, , J. David Schneider

ITER envisages the use of two heating neutral beam injectors plus an optional one as part of the auxiliary heating and current drive system. The 16.5 MW expected neutral beam power per injector is several notches higher than worldwide…

Plasma Physics · Physics 2023-04-05 D. Marcuzzi , V. Toigo , M. Boldrin , G. Chitarin , S. Dal Bello , L. Grando , A. Luchetta , R. Pasqualotto , M. Pavei , G. Serianni , L. Zanotto , R. Agnello , P. Agostinetti , M. Agostini , D. Aprile , M. Barbisan , M. Battistella , G. Berton , M. Bigi , M. Brombin , V. Candela , V. Candeloro , A. Canton , R. Casagrande , C. Cavallini , R. Cavazzana , L. Cordaro , N. Cruz , M. Dalla Palma , M. Dan , A. De Lorenzi , R. Delogu , M. De Muri , M. De Nardi , S. Denizeau , M. Fadone , F. Fellin , A. Ferro , E. Gaio , C. Gasparrini , F. Gnesotto , P. Jain , A. La Rosa , D. Lopez-Bruna , R. Lorenzini , A. Maistrello , G. Manduchi , S. Manfrin , N. Marconato , I. Mario , G. Martini , R. Milazzo , T. Patton , S. Peruzzo , N. Pilan , A. Pimazzoni , C. Poggi , N. Pomaro , B. Pouradier-Duteil , M. Recchia , A. Rigoni-Garola , D. Rizzetto , A. Rizzolo , F. Santoro , E. Sartori , B. Segalini , A. Shepherd , M. Siragusa , P. Sonato , A. Sottocornola , E. Spada , S. Spagnolo , M. Spolaore , C. Taliercio , P. Tinti , P. Tomsič , L. Trevisan , M. Ugoletti , M. Valente , M. Valisa , F. Veronese , M. Vignando , P. Zaccaria , R. Zagorski , B. Zaniol , M. Zaupa , M. Zuin , M. Cavenago , D. Boilson , C. Rotti , H. Decamps , F. Geli , A. Sharma , P. Veltri , J. Zacks , M. Simon , F. Paolucci , A. Garbuglia , D. Gutierrez , A. Masiello , G. Mico , C. Labate , P. Readman , E. Bragulat , L. Bailly-Maitre , G. Gomez , G. Kouzmenko , F. Albajar , M. Kashiwagi , H. Tobari , A. Kojima , M. Murayama , S. Hatakeyama , E. Oshita , T. Maejima , N. Shibata , Y. Yamashita , K. Watanabe , N. P. Singh , M. J. Singh , H. Dhola , U. Fantz , B. Heinemann , C. Wimmer , D. Wünderlich , K. Tsumori , G. Croci , G. Gorini , A. Muraro , M. Rebai , M. Tardocchi , L. Giacomelli , D. Rigamonti , F. Taccogna , D. Bruno , M. Rutigliano , S. Longo , S. Deambrosis , E. Miorin , F. Montagner , A. Tonti , F. Panin

CERN is now setting up String 2, a full-size prototype of a regular cell of the LHC arc. It is composed of two quadrupole, six dipole magnets, and a separate cryogenic distribution line (QRL) for the supply and recovery of the cryogen. An…

Instrumentation and Detectors · Physics 2007-05-23 A. Suraci , T. Bager , Ch. Balle , E. Blanco , J. Casas , P. Gomes , S. Pelletier , L. Serio , N. Vauthier

The MINERvA experiment is designed to make precision measurements of various neutrino cross sections in the low energy regime. We describe the detector and give the performance of some of the measured quantities.

High Energy Physics - Experiment · Physics 2010-11-05 H. Budd

SPARC_LAB is a high-brightness electron photoinjector dedicated to FEL radiation production and research on novel acceleration techniques. It has been in operation at LNF since 2005. It is composed of a newly designed brazeless 1.6-cell…

The FREIA Laboratory at Uppsala University focuses on superconducting technology and accelerator development. It actively supports the development of the European Spallation Source, CERN, and MAX IV, among others. FREIA has developed test…

The Proton Improvement Plan II (PIP-II) at Fermilab is a program of upgrades to the injection complex. At its core is the design and construction of a CW compatible, pulsed H- SRF linac. To validate the concept of the front-end of such…