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The global availability of high-intensity neutron sources is restricted by the prohibitive costs of spallation facilities and the decommissioning of aging research reactors, while compact accelerator-driven sources (CANS) are fundamentally…

Accelerator Physics · Physics 2026-02-11 Antonio Cammi , Lorenzo Loi , Andrea Missaglia , David Alesini , Hans Heinrich Braun

This design report describes the construction plans for the world's first multi-pass SRF ERL. It is a 4-pass recirculating linac that recovers the beam's energy by 4 additional, decelerating passes. All beams are returned for deceleration…

We outline the design of beam experiments for the electron linac at the Fermilab Accelerator Science and Technology (FAST) facility and for the Integrable Optics Test Accelerator (IOTA), based on synchrotron light emitted by the electrons…

The KEK 8-GeV electron / 3.5-GeV positron linac has been operated with very different beam specifications for downstream rings, KEKB, PF and PF-AR. For the reliable operation among these beam modes intelligent beam switching and beam…

Accelerator Physics · Physics 2018-09-10 K. Furukawa , A. Enomoto , N. Kamikubota , T. Kamitani , T. Matsumoto , Y. Ogawa , S. Ohsawa , K. Oide , T. Suwada

A 52MHz Radio Frequency Quadrupole (RFQ) linear accelerator (linac) is designed to serve as an initial structure for the SSC-linac system (injector into Separated Sector Cyclotron). The designed injection and output energy are 3.5 keV/u and…

Accelerator Physics · Physics 2016-09-08 Xiao Chen , He Yuan , Yuan You-Jin , Liu Yong , Xia Jia-Wen , Lu Yuan-Rong , Yuri Batygin

In the fusion experiment ITER powerful neutral beam injection (NBI) systems will be used. The NBI's core component is a negative hydrogen ion source, which is based on a modular concept. Eight cylindrical drivers, each having a volume of…

Plasma Physics · Physics 2023-04-12 Dominikus Zielke , Stefan Briefi , Ursel Fantz

The ISIS synchrotron at the Rutherford Appleton Laboratory in the UK now routinely uses a dual harmonic RF system to accelerate beam currents in excess of 230uA to run two target stations simultaneously. The acceleration in the ISIS…

Accelerator Physics · Physics 2019-10-17 Andrew Seville , David B. Allen , Ian S. K. Gardner , Robert J. Mathieson

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

We present the design and preliminary results of a prototype beam-based digital feedback system for the Interaction Point of the International Linear Collider. A custom analogue front-end processor, FPGA-based digital signal processing…

Boron neutron capture therapy is about a century old, but still current and active. In this treatment, a high absorption cross-section of boron is used for thermal neutrons and the excited state is decomposed into alpha and lithium ions.…

Accelerator Physics · Physics 2025-04-24 H. Donya , M. Umer

The linear accelerator (LINAC) at the Los Alamos Neu-tron Science Center (LANSCE) consists of Pre-buncher, Main-Buncher, low-energy beam transport (LEBT), four 201.25-MHz Drift Tube Linacs (DTLs) and forty-four 805-MHz Coupled Cavity Linacs…

Accelerator Physics · Physics 2022-11-15 Sungil Kwon , A. Archuleta , L. Castellano , C. Marchwinski , M. Prokop , P. Van Rooy , P. Torrez

We report the measurements of the fast neutron energy response in Indian Scintillator Matrix for Reactor Anti-Neutrinos (ISMRAN) detector consisting of an array of 9$\times$10 Plastic Scintillator Bars (PSBs) at BARC, Mumbai. ISMRAN is an…

Instrumentation and Detectors · Physics 2025-06-18 R. Dey , P. K. Netrakanti , D. K. Mishra , S. P. Behera , R. Sehgal , V. Jha , L. M. Pant

The work is devoted to the development of a conceptual design for a gradient spin flipper - neutron decelerator, which is the main component of a designed UCN source for a pulsed reactor. In close cooperation between the JINR group and…

Instrumentation and Detectors · Physics 2025-03-17 A. A. Popov , K. S. Osipenko , V. I. Scherbakov , A. I. Frank , G. V. Kulin , M. A. Zakharov , V. A. Kurylev , D. A. Kolomentseva

The current program at Fermilab involves the construction of a new superconducting linear accelerator (LINAC) to replace the existing warm version. The new LINAC, together with other planned improvements, is in support of proton beam…

Accelerator Physics · Physics 2023-10-03 R. Thurman-Keup , T. Folan , M. Mwaniki , S. Sas-Pawlik

Implementation and commissioning of the EPICS based control system for the ISAC radioactive beam facility was completed. The target ion source, mass separator, and low-energy beam-lines started beam production for experiments. In parallel,…

Accelerator Physics · Physics 2007-05-23 R. Keitel , D. Bishop , D. Dale , H. Hui , S. Kadantsev , M. Leross , R. Nussbaumer , J. Richards , E. Tikhomolov , G. Waters

The ICARUS liquid argon TPC detector is taking data on the Booster (BNB) and Main Injector (NuMI) Neutrino beam lines at Fermilab with a trigger system based on the scintillation light produced by charged particles in coincidence with the…

High Energy Physics - Experiment · Physics 2026-02-19 ICARUS collaboration , F. Abd Alrahman , P. Abratenko , N. Abrego-Martinez , A. Aduszkiewicz , F. Akbar , L. Aliaga Soplin , M. Artero Pons , J. Asaadi , W. F. Badgett , B. Baibussinov , F. Battisti , V. Bellini , R. Benocci , J. Berger , S. Berkman , S. Bertolucci , M. Betancourt , A. Blanchet , F. Boffelli , M. Bonesini , T. Boone , B. Bottino , A. Braggiotti , D. Brailsford , S. J. Brice , V. Brio , C. Brizzolari , H. S. Budd , A. Campani , A. Campos , D. Carber , M. Carneiro , I. Caro Terrazas , H. Carranza , F. Castillo Fernandez , S. Centro , G. Cerati , A. Chatterjee , D. Cherdack , S. Cherubini , N. Chithirasreemadam , M. Cicerchia , T. E. Coan , A. Cocco , M. R. Convery , L. Cooper-Troendle , S. Copello , H. Da Motta , M. Dallolio , A. A. Dange , A. de Roeck , S. Di Domizio , D. Di Ferdinando , L. Di Noto , M. Diwan , S. Dolan , L. Domine , S. Donati , F. Drielsma , J. Dyer , S. Dytman , A. Falcone , C. Farnese , A. Fava , N. Gallice , F. G. Garcia , C. Gatto , D. Gibin , A. Gioiosa , W. Gu , A. Guglielmi , G. Gurung , K. Hassinin , H. Hausner , A. Heggestuen , B. Howard , R. Howell , Z. Hulcher , I. Ingratta , C. James , W. Jang , Y. -J. Jwa , L. Kashur , W. Ketchum , J. S. Kim , D. -H. Koh , T. Krishnan , J. Larkin , Y. Li , C. Mariani , C. M. Marshall , S. Martynenko , N. Mauri , K. S. McFarland , A. Menegolli , G. Meng , O. G. Miranda , A. Mogan , N. Moggi , E. Montagna , A. Montanari , C. Montanari , M. Mooney , G. Moreno-Granados , J. Mueller , M. Murphy , D. P. Méndez , D. Naples , S. Palestini , M. Pallavicini , V. Paolone , L. Pasqualini , L. Patrizii , L. Paudel , G. Petrillo , C. Petta , V. Pia , F. Pietropaolo , F. Poppi , M. Pozzato , M. L. Pumo , G. Putnam , X. Qian , A. Rappoldi , G. L. Raselli , S. Repetto , F. Resnati , A. M. Ricci , E. Richards , M. Rosenberg , M. Rossella , N. Rowe , P. Roy , C. Rubbia , M. Saad , S. Saha , G. Salmoria , S. Samanta , A. Scaramelli , D. Schmitz , A. Schukraft , D. Senadheera , S-H. Seo , F. Sergiampietri , G. Sirri , J. S. Smedley , J. Smith , M. Sotgia , L. Stanco , J. Stewart , H. A. Tanaka , M. Tenti , K. Terao , F. Terranova , V. Togo , D. Torretta , M. Torti , F. Tortorici , D. Totani , R. Triozzi , Y. -T. Tsai , K. V. Tsang , T. Usher , F. Varanini , N. Vardy , S. Ventura , M. Vicenzi , C. Vignoli , B. Viren , F. A. Wieler , Z. Williams , P. Wilson , R. J. Wilson , J. Wolfs , T. Wongjirad , A. Wood , E. Worcester , M. Worcester , M. Wospakrik , J. Xia , S. Yadav , H. Yu , J. Yu , A. Zani , J. Zennamo , J. Zettlemoyer , C. Zhang , S. Zucchelli

Currently there is a Proposed FNAL 750keV Injector Upgrade for the replacement of the 40 year old Fermi National Laboratory (FNAL) Cockcroft-Walton accelerators with a new ion source and 200MHz Radio Frequency Quadruple (RFQ). The slit type…

Accelerator Physics · Physics 2012-07-31 D. S. Bollinger

LCLS-II is currently in its commissioning phase at SLAC. It is an X-ray FEL driven by a CW superconducting LINAC. The beam injector plays a crucial role in the overall performance of the accelerator, and is critical to the final electron…

CEBAF, the Continuous Electron Beam Accelerator Facility, has been actively serving the nuclear physics research community as a unique forefront international resource since 1995. This CW electron linear accelerator (linac) at the U.S.…

Accelerator Physics · Physics 2017-02-01 Charles E. Reece

Today a linear particle accelerator (linac), in which electric and magnetic fields are of vital importance, is one of the popular energy generation sources like Accelerator Driven System (ADS). A multipurpose, including primarily ADS,…

General Physics · Physics 2019-07-10 H. F. Kisoglu , M. Yilmaz
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