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The Muon g-2 experiment at Fermilab, with the aim to measure the muon anomalous magnetic moment to an unprecedented level of 140~ppb, has started beam and detector commissioning in Summer 2017. To deal with incoming data projected to be…

Instrumentation and Detectors · Physics 2019-08-14 Kim Siang Khaw

The PLS-II has a 100 MeV pre-injector for the 3 GeV Linac. A thermionic gun produces electron charge of 200 pC with a bunch duration of 500 ps by a 250 ps triggering pulser. At the pre-injector, one of the most important beam parameters to…

Accelerator Physics · Physics 2016-11-03 Byung-Joon Lee , Ilmoon Hwang , Chong do Park , SomJai Chunjarean , Changbum Kim

Unforeseen particle accelerator interruptions, also known as interlocks, lead to abrupt operational changes despite being necessary safety measures. These may result in substantial loss of beam time and perhaps even equipment damage. We…

Accelerator Physics · Physics 2023-03-17 Sichen Li , Jochem Snuverink , Fernando Perez-Cruz , Andreas Adelmann

An introduction and the status of R&D activities for a high-resolution, "cold" beam position monitor (BPM) and the related read-out electronics are discussed. Two different BPM detector concepts, to be attached to the SC quadrupole and…

Accelerator Physics · Physics 2009-02-19 M. Wendt , T. Lefevre , C. Simon , S. Vilalte

In order to ensure the beam quality and meet the requirements introduced by the BEPCII storage ring, the beam energy feedback system has been developed at the exit of the linac. This paper describes the implementation and commissioning of…

Accelerator Physics · Physics 2016-10-05 Shaozhe Wang , Yunlong Chi , Rong Liu , Xuefang Huang , Lei Qian

We report on the status of the Fermilab accelerator complex, including recent performance, upgrades in progress, and plans for the future. Beam delivery to the neutrino experiments surpassed our goals for the past year. The Proton…

Accelerator Physics · Physics 2016-12-30 M. E. Convery

The National Ignition Facility (NIF) will contain the world's most powerful laser. NIF requires more than 1500 precisely timed trigger pulses to control the timing of laser and diagnostic equipment. The Integrated Timing System applies new…

Instrumentation and Detectors · Physics 2007-05-23 R. A. Lerche , G. W. Coutts , L. J. Lagin , R. A. Nyholm , N. R. Sewall , R. D. Stever , J. D. Wiedwald , J. Larkin , S. Stein , R. Martin

High-energy laser facilities such as PHELIX at GSI require excellent beam pointing stability for reproducibility and relative independence for future experiments. Beam pointing stability has been traditionally achieved using simple…

Swift, high resolution CMOS pixel sensors are being developed for the ILC vertex detector, aiming to allow approaching the interaction point very closely. A major issue is the time resolution of the sensors needed to deal with the high…

Magnet power supplies in the PSI accelerator complex with their control and field-bus are old. Some components are more then 30 years old. To guarantee further maintenance and to meet the more demanding specifications for operation with the…

Accelerator Physics · Physics 2010-01-15 D. Anicic , T. Blumer , G. Dzieglewski , G. Janser , I. Jirousek , H. Lutz , A. C. Mezger

The accelerator for the APT Project is a 100 mA CW proton linac with an output energy of 1030 MeV. A High Energy Beam Transport (HEBT) conveys the beam to a raster expander, that provides a large rectangular distribution at a target/blanket…

Accelerator Physics · Physics 2008-11-26 J. F. Tooker , R. Bourque , D. Christiansen , J. Kamperschroer , G. Laughon , M. McCarthy , M. Schulze

A disruption mitigation system (DMS) is necessary for fusion-grade tokamaks like ITER in order to ensure the preservation of machine components throughout their designated operational lifespan. To address the intense heat and…

Plasma Physics · Physics 2023-12-07 Anshkumar Himanshu Patel

We propose an evolution of the Mu2e experiment, called Mu2e-II, that would leverage advances in detector technology and utilize the increased proton intensity provided by the Fermilab PIP-II upgrade to improve the sensitivity for…

Instrumentation and Detectors · Physics 2018-02-09 F. Abusalma , D. Ambrose , A. Artikov , R. Bernstein , G. C. Blazey , C. Bloise , S. Boi , T. Bolton , J. Bono , R. Bonventre , D. Bowring , D. Brown , D. Brown , K. Byrum , M. Campbell , J. -F. Caron , F. Cervelli , D. Chokheli , K. Ciampa , R. Ciolini , R. Coleman , D. Cronin-Hennessy , R. Culbertson , M. A. Cummings , A. Daniel , Y. Davydov , S. Demers , D. Denisov , S. Denisov , S. Di Falco , E. Diociaiuti , R. Djilkibaev , S. Donati , R. Donghia , G. Drake , E. C. Dukes , B. Echenard , A. Edmonds , R. Ehrlich , V. Evdokimov , P. Fabbricatore , A. Ferrari , M. Frank , A. Gaponenko , C. Gatto , Z. Giorgio , S. Giovannella , V. Giusti , H. Glass , D. Glenzinski , L. Goodenough , C. Group , F. Happacher , L. Harkness-Brennan , D. Hedin , K. Heller , D. Hitlin , A. Hocker , R. Hooper , G. Horton-Smith , C. Hu , P. Q. Hung , E. Hungerford , M. Jenkins , M. Jones , M. Kargiantoulakis , K. S. Khaw , B. Kiburg , Y. Kolomensky , J. Kozminski , R. Kutschke , M. Lancaster , D. Lin , I. Logashenko , V. Lombardo , A. Luca , G. Lukicov , K. Lynch , M. Martini , A. Mazzacane , J. Miller , S. Miscetti , L. Morescalchi , J. Mott , S. E. Mueller , P. Murat , V. Nagaslaev , D. Neuffer , Y. Oksuzian , D. Pasciuto , E. Pedreschi , G. Pezzullo , A. Pla-Dalmau , B. Pollack , A. Popov , J. Popp , F. Porter , E. Prebys , V. Pronskikh , D. Pushka , J. Quirk , G. Rakness , R. Ray , M. Ricci , M. Röhrken , V. Rusu , A. Saputi , I. Sarra , M. Schmitt , F. Spinella , D. Stratakis , T. Strauss , R. Talaga , V. Tereshchenko , N. Tran , R. Tschirhart , Z. Usubov , M. Velasco , R. Wagner , Y. Wang , S. Werkema , J. Whitmore , P. Winter , L. Xia , L. Zhang , R. -Y. Zhu , V. Zutshi , R. Zwaska

Injected beam energy and energy spread are critical parameters affecting the performance of our rapid cycling synchrotron (RCS). A real-time energy monitoring system is being installed to examine the H- beam out of the Intense Pulsed…

Accelerator Physics · Physics 2009-09-25 J. C. Dooling , F. R. Brumwell , M. K. Lien , G. E. McMichael

The Project X Injector Experiment (PXIE) will serve as a prototype for the Project X front end. The aim is to validate the Project-X design and to decrease technical risks, known to be mainly related to the front end. PXIE will accelerate a…

Accelerator Physics · Physics 2013-01-31 V. A. Lebedev , S. Nagaitsev , J. -F. Ostiguy , A. V. Shemyakin , B. G. Shteynas , N. Solyak , N. Solyak

The Fermilab Linac delivers 400 MeV H- beam to the rest of the accelerator chain. Providing stable intensity, energy, and emittance is key since it directly affects downstream machines. To operate high current beam, accelerators must…

Accelerator Physics · Physics 2023-07-11 R. Sharankova , M. Mwaniki , K. Seiya , M. Wesley

The peak current limit for the Fermilab Linac was recently studied. The purpose was to learn what components of the present Linac can be used for the first stage of a proposed proton driver[1]. For this application the Linac must provide a…

Accelerator Physics · Physics 2007-05-23 M. Popovic , L. Allen , A. Moretti , E. McCrory , C. W. Schmidt , T. Sullivan

A dielectric-loaded linac powered by THz-pulses is one of the key parts of the "Attosecond X-ray Science: Imaging and Spectroscopy" (AXSIS) project at DESY, Hamburg. As in conventional accelerators, the AXSIS linac is designed to have phase…

Accelerator Physics · Physics 2018-12-26 K. Galaydych , R. Assmann , U. Dorda , B. Marchetti , G. Vashchenko , I. Zagorodnov

The Fermi National Accelerator Laboratory (Fermilab) Linac accepts 750 keV H- ions from the front end and accelerates them to 400 MeV for injection into the Booster rapid cycling synchrotron. Day-to-day drifts in the beam longitudinal…

Accelerator Physics · Physics 2024-07-25 R. Sharankova , A. Shemyakin , S. Rego

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