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This paper describes the concept of a primary electron beam facility at CERN, to be used for dark gauge force and light dark matter searches. The electron beam is produced in three stages: A Linac accelerates electrons from a photo-cathode…

Accelerator Physics · Physics 2019-05-21 T. Åkesson , R. Corsini , Y. Dutheil , L. Evans , B. Goddard , A. Grudiev , A. Latina , Y. Papaphilippou , S. Stapnes

Fermilab is committed to upgrading its accelerator complex towards the intensity frontier to pursue HEP research in the neutrino sector and beyond. The upgrade has two steps: 1) the Proton Improvement Plan (PIP), which is underway, has its…

Accelerator Physics · Physics 2017-05-04 C. M. Bhat

The possibility of using electron beam phase space manipulations to support a free-electron laser accelerator design optimization has motivated our research. An on-going program demonstrating the exchange of transverse horizontal and…

Accelerator Physics · Physics 2012-08-10 A. H. Lumpkin , A. S. Johnson , J. Ruan , J. Santucci , Y. -E. Sun , R. Thurman-Keup , H. Edwards

The performance of a particle accelerator can be limited by the build-up of an electron cloud (EC) in the vacuum chamber. Secondary electron emission from the chamber walls can contribute to EC growth. An apparatus for in-situ measurements…

The Japan Proton Accelerator Research Complex (J-PARC) currently delivers a 1 MW, 3 GeV proton beam to the Materials and Life Science Experimental Facility (MLF). Power is expected to increase to 1.3 MW, driven by the needs of…

Cornell's electron/positron storage ring (CESR) was modified over a series of accelerator shutdowns beginning in May 2008, which substantially improves its capability for research and development for particle accelerators. CESR's energy…

Accelerator Physics · Physics 2015-09-02 M. G. Billing

A new CLIC Test Facility (CTF3) at CERN will serve to study the drive beam generation for the Compact Linear Collider (CLIC). CTF3 has to accelerate a 3.5 A electron beam in almost fully-loaded structures. The pulse contains more than 2000…

Accelerator Physics · Physics 2010-11-15 D. Schulte

The upgrade of the ALICE TPC will allow the experiment to cope with the high interaction rates foreseen for the forthcoming Run 3 and Run 4 at the CERN LHC. In this article, we describe the design of new readout chambers and front-end…

Instrumentation and Detectors · Physics 2021-03-26 J. Adolfsson , M. Ahmed , S. Aiola , J. Alme , T. Alt , W. Amend , F. Anastasopoulos , C. Andrei , M. Angelsmark , V. Anguelov , A. Anjam , H. Appelshäuser , V. Aprodu , O. Arnold , M. Arslandok , D. Baitinger , M. Ball , G. G. Barnaföldi , E. Bartsch , P. Becht , R. Bellwied , A. Berdnikova , M. Berger , N. Bialas , P. Bialas , S. Biswas , B. Blidaru , L. Boldizsár , L. Bratrud , P. Braun-Munzinger , M. Bregant , C. L. Britton , S. Brucker , E. J. Brücken , H. Büsching , R. Soto Camacho , A. L. Campos , G. Caragheorgheopol , D. D. Carvalho , A. J. Castro , P. Chatzidaki , P. Christiansen , L. G. Clonts , T. M. Cormier , A. L. D. Couto , H. G. A. Cubas , A. Deisting , P. Dhankher , S. Dittrich , V. Duta , R. Ehlers , M. Engel , M. N. Ericson , N. B. Ezell , L. Fabbietti , F. Flor , G. Föhner , U. Frankenfeld , E. Futo , J. J. Gaardhøje , M. G. Munhoz , C. Garabatos , P. Gasik , T. Geiger , Á. Gera , P. Glässel , D. J. Q. Goh , O. Grachov , A. Grein , M. Gul , T. Gunji , M. Habib , H. Hamagaki , G. Hamar , J. C. Hansen , A. Harlenderova , J. W. Harris , S. Hassan , P. Hauer , S. Hayashi , S. T. Heckel , J. Hehner , J. K. Heino , E. Hellbär , H. Helstrup , A. Herghelegiu , L. Hernandes da Costa Porto , R. A. Hernandez , H. D. Hernandez Herrera , T. Herold , T. E. Hilden , B. Hohlweger , S. Hornung , C. Hughes , S. Hummel , M. Ivanov , J. Jung , M. Jung , D. Just , E. Kangasaho , L. Karayan , B. Ketzer , S. Kirsch , M. Kleiner , T. Klemenz , S. Klewin , A. G. Knospe , E. Koskinen , M. Kowalski , L. Kreis , M. Krüger , N. Kupfer , R. Lang , L. Lautner , M. Lesch , Y. Lesenechal , F. Liebske , C. Lippmann , V. Litichevskyi , M. Ljunggren , W. J. Llope , S. Mahmood , T. Mahmoud , R. D. Majka , C. Markert , J. Martinez , T. A. Martins , S. Masciocchi , A. Mathis , O. Matonoha , Y. Matsuyama , A. Matyja , M. Meres , D. L. Mihaylov , D. Miśkowiec , T. Mittelstaedt , L. S. Montali , D. M. Moraes , C. Mordasini , T. Morhardt , S. Muley , J. Mulligan , R. H. Munzer , H. Murakami , K. Münning , A. Nassirpour , H. Natal da Luz , C. Nattrass , R. A. Negrao De Oliveira , H. G. Neves , B. S. Nielsen , W. A. V. Noije , M. Ogino , A. C. Oliveira Da Silva , A. Oskarsson , J. Ottnad , K. Oyama , A. Önnerstad , L. Österman , A. A. Pabon , Y. Pachmayer , G. Paić , J. Parkkila , S. Pathak , R. N. Patra , V. Peskov , M. Petris , M. Petrovici , M. Planinic , F. Pompei , L. Prodan , A. Radu , L. Radulescu , J. Rak , J. Rasson , V. Ratza , K. F. Read , A. Rehman , R. Renfordt , K. Røed , D. Röhrich , E. Rubio , T. Rudzki , A. Rusu , M. Saleh , B. C. S. Sanches , J. Schambach , S. Scheid , C. Schmidt , A. Schmier , H. Schulte , K. Schweda , D. Sekihata , N. Shimizu , S. Siebig , R. W. D. Silva , D. Silvermyr , D. Simpson , B. Sitar , N. Smirnov , T. Snellman , H. K. Soltveit , S. P. Sorensen , F. Sozzi , J. Stachel , A. Szabo , L. Šerkšnytė , Y. Takeuchi , G. Tambave , Y. Tanaka , K. Terasaki , R. J. Turpeinen , K. Ullaland , B. Ulukutlu , E. Umaka , A. Utrobicic , D. Varga , A. Vargas , M. Vargyas , R. Varma , O. Vazquez Rueda , A. Velure , S. Vereschagin , S. Vergara Limón , L. Vergara Urrutia , O. Vorbach , B. Voss , D. Vranic , R. J. Warmack , T. O. Weber , C. Weidlich , J. Wiechula , B. Windelband , S. Winkler , W. Witt

Fermilab is upgrading its Booster synchrotron to increase ramp rate and intensity. This is part of the Proton Improvement Plan (PIP-II) that will allow the Main Injector to achieve proton beam power of 1.2 MW within the next few years. This…

The Tevatron Run-II program has been in progress since 2001, and the CDF and D0 experiments have been operational with upgraded detectors. Coupled with recent improvements in the Tevatron accelerator performance, the experiments have…

High Energy Physics - Experiment · Physics 2019-08-14 Fumihiko Ukegawa

This document describes the concept of a primary electron beam facility at CERN, to be used for dark gauge force and light dark matter searches. The electron beam is produced in three stages: A Linac accelerates electrons from a…

Accelerator Physics · Physics 2018-06-01 T. Åkesson , Y. Dutheil , L. Evans , A. Grudiev , Y. Papaphilippou , S. Stapnes

The Forward Detector upgrade project at CDF is designed to enhance the capabilities for studies of diffractive physics at the Tevatron during Run II. Studies of hard diffraction and very forward physics are some of the topics that can be…

High Energy Physics - Experiment · Physics 2007-05-23 Michele Gallinaro

The multi-stage method of laser wakefield acceleration (LWFA) presents a promising approach for developing stable, full-optical, high-energy electron accelerators. By segmenting the acceleration process into several booster stages, each…

Plasma Physics · Physics 2025-02-17 Srimanta Maity , Pavel Sasorov , Alexander Molodozhentsev

A high energy beam absorber has been built for the Advanced Superconducting Test Accelerator (ASTA) at Fermilab. In the facility's initial configuration, an electron beam will be accelerated through 3 TTF-type or ILC-type RF cryomodules to…

Accelerator Physics · Physics 2013-01-24 C. Baffes , M. Church , J. Leibfritz , S. Oplt , I. Rakhno

Currently, Fermilab Booster accelerates ~4.5E12 protons per pulse (ppp) in 81 bunches from 400 MeV to 8 GeV at 15 Hz to provide beam to multiple HEP experiments and is being upgraded to handle higher beam intensity >6.7E12 ppp at a…

Accelerator Physics · Physics 2021-10-20 C. M. Bhat , N. Eddy

The upgraded Facility for Advanced Accelerator Experimental Tests (FACET-II) at SLAC National Accelerator Laboratory has been designed to deliver ultra-relativistic electron and positron beams with unprecedented parameters, especially in…

The Edwards Accelerator Laboratory at Ohio University is the hub for a vibrant program in low energy nuclear physics. Research performed with the lab's 4.5MV tandem accelerator spans a variety of topics, including nuclear astrophysics,…

Instrumentation and Detectors · Physics 2017-10-31 Zach Meisel , C. R. Brune , S. M. Grimes , D. C. Ingram , T. N. Massey , A. V. Voinov

The Hybrid Asymmetric Linear Higgs Factory (HALHF) proposes a shorter and cheaper design for a future Higgs factory. It reaches a $\sqrt{s} = 250$ GeV using a 500 GeV electron beam accelerated by an electron-driven plasma wake-field, and a…