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Radio-frequency linear accelerators are used as injectors for synchrotrons and as stand-alone accelerators for the production of intense particle beams, thanks to their ability to accelerate high beam currents at high repetition rates. This…

Accelerator Physics · Physics 2013-03-28 Maurizio Vretenar

The CLIC study of a high-energy (0.5 - 5 TeV), high-luminosity (1034 - 1035 cm-2 sec-1) e+e- linear collider is presented. Beam acceleration using high frequency (30 GHz) normal-conducting structures operating at high accelerating fields…

Accelerator Physics · Physics 2008-11-26 Jean-Pierre Delahaye , Ian Wilson

Spallation source dedicated for neutron scattering experiments, as well as multi-purpose facilities serving several applications call for pulsed mode operation of a high intensity proton linac. There is general agreement on the…

Accelerator Physics · Physics 2007-05-23 Alban Mosnier

Project-X is a leading candidate of the next major accelerator construction project at Fermilab. The mission need of Project-X is to establish an intensity frontier for particle physics research, or more precisely, to build a multi-MW…

Accelerator Physics · Physics 2009-12-16 W. Chou

The China spallation neutron source (CSNS) linac is designed with beam energy of 81MeV and a peak current of 15mA in the first phase. The RF power system for the 81 MeV Linac requires 8 units of RF power sources, each unit has one…

Accelerator Physics · Physics 2019-09-26 Linyan Rong , Zhencheng Mu , Zhexin Xie , Bo Wang , Wenzhong Zhou , Maliang Wan , Meifei Liu , Jian Li , Xinan Xu

In this study, a low energy beam transport (LEBT) channel for the proton linac section of the Turkish Accelerator Center (TAC) has been designed by using TRAVEL code. Commonly used LEBT including two focusing solenoid magnets will transport…

Accelerator Physics · Physics 2014-05-29 H. F. Kisoglu , A. Caliskan , S. Sultansoy , M. Yilmaz

For the CLIC two-beam scheme, a high-current, long-pulse drive beam is required for RF power generation. Taking advantage of the 3 GHz klystrons available at the LEP injector once LEP stops, a 180 MeV electron accelerator is being…

Accelerator Physics · Physics 2007-05-23 G. Carron , E. Jensen , M. Luong , A. Millich , E. Rugo , I. Syratchev , L. Thorndahl

The Proton Improvement Plan-II (PIP-II) [1] has been developed at Fermilab to provide powerful proton beams to the laboratorys experiments. An 800-MeV superconducting linear accelerator-a centerpiece of the project-is currently under…

Accelerator Physics · Physics 2023-01-23 Igor Rakhno , Nikolai Mokhov , Igor Tropin , Sergei Striganov , Yury Eidelman

As the pre-injector of the LHC injector chain, the proton linac at CERN is required to provide a high-intensity (180mA) beam to the Proton Synchrotron Booster. The results of measurements at this intensity will be presented. Furthermore,…

Accelerator Physics · Physics 2007-05-23 C. E. Hill , A. Lombardi , R. Scrivens , M. Vretenar , A. Feschenko , A. Liou

The superconducting (SC) proton linac is proposed in the JAERI/KEK Joint Project for a high-intensity proton accelerator in the energy region from 400 to 600 MeV. Highly stable fields in the SC cavities are required under the dynamic…

Accelerator Physics · Physics 2019-08-17 N. Ouchi , E. Chishiro , C. Tsukishima , K. Mukugi

The Proton Improvement Plan - II (PIP-II) injector linac is an 800 MeV superconducting H$^-$ linac, christened Linac2, that will replace the existing 400 MeV injector to the accelerator complex at Fermilab. The higher energy, intensity and…

Accelerator Physics · Physics 2026-05-12 S. Krishnagopal , M. Convery , J. Dey

The article considers a proton accelerator containing seven independent beams arranged on the accelerator radius. The current in each beam is one hundred milliamps. The initial part of the accelerator consists of shielded spiral waveguides…

Accelerator Physics · Physics 2015-09-15 S. N. Dolya

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

Suppression of beam losses is essential for successful operation of high-intensity linac. Historically, the values of the field amplitudes and phases of the side-coupled, 805-MHz LANSCE linac modules are maintained using a well-known…

Accelerator Physics · Physics 2020-02-26 Y. K. Batygin , F. E. Shelley , H. A. Watkins

As a part of the ongoing XIIth plan project titled "R&D activities for high energy proton linac based spallation neutron source", the work on physics design of various subsystems of the injector linac and accumulator ring has been taken up…

The treatment of flue gases from power plants and municipal or industrial wastewater using electron beam irradiation technology has been successfully demonstrated in small-scale pilot plants. The beam energy requirement is rather modest, on…

The conception of High Power Linac developed in Russian accelerator centres is based on the use of independently phased SC resonators with quadrupole lenses between them. The type and parameters of the resonators as well as focusing…

Accelerator Physics · Physics 2007-05-23 A. Kolomiets , S. Yaramishev

The Circular Electron Positron Collider (CEPC) is a large scientific project initiated and hosted by China, fostered through extensive collaboration with international partners. The complex comprises four accelerators: a 30 GeV Linac, a 1.1…

Accelerator Physics · Physics 2026-01-27 The CEPC Study Group

The LIGHT (Linac for Image-Guided Hadron Therapy) project was initiated to develop a modular proton accelerator delivering beam with energies up to 230 MeV for cancer therapy. The machine consists of three different kinds of accelerating…

Front end of a CW linac of the Project X contains an H source, an RFQ, a medium energy transport line with the beam chopper, and a SC low-beta linac that accelerates H- from 2.5 MeV to 160 MeV. SC Single Spoke Resonators (SSR) will be used…

Accelerator Physics · Physics 2012-02-13 T. Khabiboulline , S. Barbanotti , I. Gonin , N. Solyak , I. Terechkine , V. Yakovlev