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Related papers: Overview of the APT Accelerator Design

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For many next-generation high intensity proton accelerator applications including the Spallation Neutron Source (SNS), superconducting (SC) RF provides the technology of choice for the linac. In designing the superconducting cavity, several…

Accelerator Physics · Physics 2007-05-23 Sang-ho Kim , Marc Doleans , Yoon Kang

We have developed high-efficiency normal-conducting RF accelerating structures by combining H-mode resonator cavities and a transverse beam focusing by permanent-magnet quadrupoles (PMQ), for beam velocities in the range of a few percent of…

Accelerator Physics · Physics 2011-04-20 Sergey S. Kurennoy , Lawrence J. Rybarcyk , James F. O'Hara , Eric R. Olivas , Thomas P. Wangler

To realize and test advanced accelerator concepts and hardware, a beamline is being reconfigured in the Linac Extension Area (LEA) of APS linac. A photo-cathode RF gun installed at the beginning of the APS linac will provide a low emittance…

Accelerator Physics · Physics 2018-06-20 Seunghwan Shin , Yine Sun , Jeff Dooling , Alexander Zholents

This paper presents SleepViT, a custom accelerator ASIC for real-time, low-power sleep stage classification in wearable devices. At the core of SleepViT is a lightweight vision transformer model specifically optimized for…

Signal Processing · Electrical Eng. & Systems 2025-09-08 Tristan Robitaille , Xilin Liu

The U.S. Particle Physics Project Prioritization Panel (P5) report encouraged the realization of Fermilab's Proton Improvement Plan II (PIP-II) to support future neutrino programs in the United States. PIP-II aims at enhancing the…

Accelerator Physics · Physics 2017-01-05 A. Vivoli

The completion of the PIP-II project and its superconducting linear accelerator will provide up to 1.2 MW of beam power to the LBNF/DUNE facility for neutrino physics. It will also be able to produce high-power beams directly from the linac…

This paper begins with a summary of the status of the Large Hadron Collider at CERN, including the lead-ion injector chain and the plans for the first phases of commissioning and operation with colliding proton beams. In a later phase, the…

Nuclear Experiment · Physics 2011-09-02 John M. Jowett

The superconducting upgrade of the REX-ISOLDE radioactive ion beam (RIB) post-accelerator at CERN will utilise a compact lattice comprising quarter-wave resonators (QWRs) and solenoids, accelerating beams in the mass range 2.5 < A/q < 4.5…

Accelerator Physics · Physics 2009-09-29 M. A. Fraser , M. Pasini , A. D'Elia , R. M. Jones

The warm front end of the PIP2IT accelerator, assem-bled and commissioned at Fermilab, consists of a 15 mA DC, 30 keV H- ion source, a 2 m long Low Energy Beam Transport (LEBT) line, and a 2.1 MeV, 162.5 MHz CW RFQ, followed by a 10 m long…

RF power coupler is a key component of the superconducting accelerating system in Chinese ADS proton linac injector I, which is used to transmit 15kW RF power from the power source to the superconducting HWR cavity. According to the…

Accelerator Physics · Physics 2013-12-06 Fanbo Meng , Xu Chen , Weimin Pan , Tongming Huang , Qiang Ma , Haiying Lin , Xiaohua Peng

At the Ibaraki Neutron Medical Research Center, an accelerator-based neutron source for iBNCT (Ibaraki - Boron Neutron Capture Therapy) is being developed using an 8-MeV proton linac and a beryllium-based neutron production target. The…

The Proton Improvement Plan - II (PIP-II) is a new linear accelerator (LINAC) complex being built at Fermilab. It is based on superconducting radiofrequency cavities and will accelerate H- ions to 800 MeV kinetic energy before injection…

Accelerator Physics · Physics 2023-10-05 R. Thurman-Keup , M. El Baz , V. Scarpine

The Compact Linear Collider (CLIC) is a high-energy high-luminosity linear electron-positron collider under development. It is foreseen to be built and operated in three stages, at centre-of-mass energies of 380 GeV, 1.5 TeV and 3 TeV,…

Instrumentation and Detectors · Physics 2019-05-08 A. C. Abusleme Hoffman , G. Parès , T. Fritzsch , M. Rothermund , H. Jansen , K. Krüger , F. Sefkow , A. Velyka , J. Schwandt , I. Perić , L. Emberger , C. Graf , A. Macchiolo , F. Simon , M. Szalay , N. van der Kolk , H. Abramowicz , Y. Benhammou , O. Borysov , M. Borysova , A. Joffe , S. Kananov , A. Levy , I. Levy , G. Eigen , R. Bugiel , S. Bugiel , M. Firlej , T. A. Fiutowski , M. Idzik , J. Moroń , K. P. Świentek , P. Terlecki , P. Brückman de Renstrom , B. Turbiarz , T. Wojtoń , L. K. Zawiejski , E. Firu , V. Ghenescu , A. T. Neagu , T. Preda , I. Boyko , Yu. Nefedov , A. Rymbekova , A. Sapronov , G. Shelkov , A. Zhemchugov , A. Ruiz-Jimeno , I. Vila , E. Fullana , J. Fuster , P. Gomis Lopez , M. Perelló , M. A. Villarejo , M. Vos , J. Alozy , N. Alipour Tehrani , D. Arominski , R. Ballabriga Sune , F. Boyer , E. Brondolin , M. Buckland , M. Campbell , D. Dannheim , K. Dette , F. Duarte Ramos , N. Egidos Plaja , K. Elsener , A. Fiergolski , C. Fuentes Rojas , C. Grefe , D. Hynds , W. Klempt , I. Kremastiotis , J. Kröger , S. Kulis , E. Leogrande , L. Linssen , X. Llopart Cudie , A. Lucaci-Timoce , M. Munker , L. Musa , A. Nürnberg , F. -X. Nuiry , E. Perez Codina , H. Pernegger , M. Petrič , F. Pitters , T. Quast , S. Redford , P. Riedler , P. Roloff , A. Sailer , E. Santin , U. Schnoor , E. Sicking , K. Sielewicz , R. Simoniello , W. Snoeys , S. Spannagel , S. Sroka , R. Ström , P. Valerio , S. van Dam , E. van der Kraaij , T. Vǎnát , O. Viazlo , M. Vicente Barreto Pinto , M. A. Weber , M. Williams , K. Wolters , M. Benoit , G. Iacobucci , D M S Sultan , R. R. Bosley , T. Price , M. F. Watson , N. K. Watson , A. G. Winter , J. Goldstein , S. Green , J. S. Marshall , M. A. Thomson , B. Xu , G. Casse , J. Vossebeld , T. Coates , F. Salvatore , J. Repond , L. Xia , C. Kenney , A. Tomada

The design and production studies of the proton beamline of SPP, which aims to acquire know-how on proton accelerator technology thru development of man power and serves as particle accelerator technologies test bench, continue at…

A test of the acceleration of multiple charge-state uranium beams was performed at the ATLAS accelerator. A 238U+26 beam was accelerated in the ATLAS PII linac to 286 MeV (~1.2 MeV/u) and stripped in a carbon foil located 0.5 m from the…

Accelerator Physics · Physics 2007-05-23 P. N. Ostroumov , R. C. Pardo , G. P. Zinkann , K. W. Shepard , J. A. Nolen

The readout electronics of the ATLAS Hadronic Endcap Calorimeter will have to withstand the about ten times larger radiation environment of the future high-luminosity LHC (HL-LHC) compared to their design values. The GaAs ASIC which…

Instrumentation and Detectors · Physics 2016-11-17 Sven Menke

The Linac Coherent Light Source (LCLS) at Stanford Linear Accelerator Center (SLAC) is in the process of being upgraded to a superconducting radio frequency (SRF) accelerator and renamed LCLS-II. This upgrade requires thirty five 1.3 GHz…

Accelerator Physics · Physics 2018-07-04 Andrew Dalesandro , Joshua Kaluzny , Arkadiy Klebaner

The LHeC is the project for delivering electron-nucleon collisions at CERN using the HL-LHC beams. An Energy Recovery Linac in racetrack configuration will provide 50 GeV electrons to achieve centre-of-mass energies around 1 TeV/nucleon and…

An electron/positron linear collider with a center-of-mass energy between 0.5 and 1 TeV would be an important complement to the physics program of the LHC in the next decade. The Next Linear Collider (NLC) is being designed by a US…

Accelerator Physics · Physics 2009-11-06 T. O. Raubenheimer
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