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Related papers: Pulsed SC Proton Linac

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To improve RHIC luminosity for heavy ion beam energies below 10 GeV/nucleon, the Low Energy RHIC electron Cooler (LEReC) is currently under commissioning at BNL. The Linac of LEReC is designed to deliver a 1.6 MeV to 2.6 MeV electron beam,…

A 5-MeV RFQ designed for a proton current up to 100-mA CW is now under construction as part of the High Intensity Proton Injector project (IPHI). Its computed transmission is greater than 99 %. The main goals of the project are to verify…

The construction of the initial part of a normally conducting linac for hydrogen ion beams with a pulsed current of ~20 mA up to an energy of ~70 MeV is considered. The RFQ at a frequency of ~160 MHz accelerates ions to an energy of ~4 MeV.…

Accelerator Physics · Physics 2023-09-21 V. V. Paramonov , A. P. Durkin , L. Yu. Ovchinnikova , I. V. Rybakov

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

Theoretical work predicts that the strong dependence of Tc on pure shear strain within the a-b plane of optimally doped YBa2Cu3O{7-delta} results in heterogenous columnar pins of vortex lines about dislocation lines and about nano-columns…

Superconductivity · Physics 2009-10-06 J. P. Rodriguez , E. J. Oswald

In proton therapy, depth scanning of the irradiated object is performed by changing the Output Energy (OE) of the accelerated beam. In pulsed linear accelerators, adjustment of the OE is usually by changing the amplitude and/or phase of the…

Accelerator Physics · Physics 2023-10-09 L. Yu. Ovchinnikova , A. P. Durkin , A. S. Kurilik , V. V. Paramonov

An S-band linear accelerator is the source of particles and the front end of the Advanced Photon Source injector. In addition, it supports a low-energy undulator test line (LEUTL) and drives a free-electron laser (FEL). A…

Accelerator Physics · Physics 2019-08-17 A. E. Grelick , N. Arnold , S. Berg , D. Dohan , G. Goeppner , Y. W. Kang , A. Nassiri , S. Pasky , G. Pile , T. Smith , S. J. Stein

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 Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear $e^+e^-$ collider under development by international collaborations hosted by CERN. This document provides an overview of the design, technology, and implementation…

Accelerator Physics · Physics 2019-03-22 M. Aicheler , P. N. Burrows , N. Catalan , R. Corsini , M. Draper , J. Osborne , D. Schulte , S. Stapnes , M. J. Stuart

The Pohang Accelerator Laboratory operates an electron linac for the pulsed neutron source as one of the long-term nuclear R&D programs at the Korea Atomic Energy Research Institute. The designed beam parameters are as follows; The nominal…

Accelerator Physics · Physics 2008-11-26 G. N. Kim , H. S. Kang , Y. S. Lee , M. H. Cho , I. S. Ko , W. Namkung

This note describes two versatile accelerator complexes that could be built at a Future Circular Collider (FCC) in order to produce $e^{+}e^{-}$, $\gamma\gamma$ and $ep$ collisions. The first facility is an SLC-type machine comprising a…

Accelerator Physics · Physics 2019-08-15 Radoje Belusevic

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

A concept for a two-stage injection-locked CW magnetron intended to drive Superconducting Cavities (SC) for intensity-frontier accelerators has been proposed. The concept considers two magnetrons in which the output power differs by 15-20…

The Fermi National Accelerator Laboratory (FNAL) Linac has been in operation for 52 years. In approximately four years, it will be replaced by a new 800 MeV superconducting machine, the PIP-II SRF Linac. In the current configuration, the…

A timely and long-term programme of kaon decay measurements at a new level of precision is presented, leveraging the capabilities of the CERN Super Proton Synchrotron (SPS). The proposed programme is firmly anchored on the experience built…

High Energy Physics - Experiment · Physics 2022-12-01 E. Cortina Gil , J. Jerhot , N. Lurkin , T. Numao , B. Velghe , V. W. S. Wong , D. Bryman , L. Bician , Z. Hives , T. Husek , K. Kampf , M. Koval , A. T. Akmete , R. Aliberti , V. Büscher , L. Di Lella , N. Doble , L. Peruzzo , M. Schott , H. Wahl , R. Wanke , B. Döbrich , L. Montalto , D. Rinaldi , F. Dettori , A. Cardini , A. Lai , L. Bomben , S. Carsi , M. Prest , A. Selmi , G. Lezzani , P. Monti-Guarnieri , L. Perna , P. Dalpiaz , V. Guidi , A. Mazzolari , I. Neri , F. Petrucci , M. Soldani , L. Bandiera , A. Cotta Ramusino , A. Gianoli , M. Romagnoni , A. Sytov , M. Lenti , I. Panichi , G. Ruggiero , A. Bizzeti , F. Bucci , A. Antonelli , E. Di Meco , G. Lanfranchi , S. Martellotti , M. Martini , M. Moulson , D. Paesani , I. Sarra , T. Spadaro , G. Tinti , E. Vallazza , F. Ambrosino , R. Giordano , P. Massarotti , M. Napolitano , G. Saracino , C. Di Donato , G. D'Ambrosio , M. D'Errico , M. Mirra , S. Neshatpour , R. Fiorenza , I. Rosa , D. De Salvador , F. Sgarbossa , G. Anzivino , S. Germani , R. Volpe , P. Cenci , S. Cutini , V. Duk , P. Lubrano , M. Pepe , M. Piccini , F. Costantini , S. Donati , M. Giorgi , S. Giudici , G. Lamanna , E. Pedreschi , J. Pinzino , M. Sozzi , R. Fantechi , V. Giusti , F. Spinella , I. Mannelli , M. Raggi , A. Biagioni , P. Cretaro , O. Frezza , F. Lo Cicero , A. Lonardo , M. Turisini , P. Vicini , R. Ammendola , V. Bonaiuto , A. Fucci , A. Salamon , F. Sargeni , R. Arcidiacono , B. Bloch-Devaux , E. Menichetti , E. Migliore , C. Biino , F. Marchetto , D. Baigarashev , Y. Kambar , D. Kereibay , Y. Mukhamejanov , S. Sakhiyev , A. Briano Olvera , J. Engelfried , N. Estrada-Tristan , R. Piandani , M. A. Reyes Santos , K. A. Rodriguez Rivera , P. C. Boboc , A. M. Bragadireanu , S. A. Ghinescu , O. E. Hutanu , T. Blazek , V. Cerny , A. Kleimenova , Z. Kucerova , D. Martinez Santos , C. Prouve , M. Boretto , F. Brizioli , A. Ceccucci , M. Corvino , H. Danielsson , F. Duval , E. Gamberini , R. Guida , E. B. Holzer , B. Jenninger , G. Lehmann Miotto , P. Lichard , K. Massri , E. Minucci , M. Perrin-Terrin , V. Ryjov , J. Swallow , M. Van Dijk , M. Zamkovsky , R. Marchevski , A. Gerbershagen , J. R. Fry , F. Gonnella , E. Goudzovski , J. Henshaw , C. Kenworthy , C. Lazzeroni , C. Parkinson , A. Romano , J. Sanders , A. Shaikhiev , A. Tomczak , H. Heath , D. Britton , A. Norton , D. Protopopescu , J. B. Dainton , R. W. L. Jones , A. De Santo , F. Salvatore , P. Cooper , D. Coward , P. Rubin

The Future Circular Collider study is exploring possible designs of circular colliders for the post-LHC era, as recommended by the European Strategy Group for High Energy Physics. One such option is FCC-hh, a proton-proton collider with a…

We present a theory describing the superconducting (SC) interaction of Dirac electrons in a quasi-two-dimensional system consisting of a stack of N planes. The occurrence of a SC phase is investigated both at T = 0 and T 5 0. At T = 0, we…

Strongly Correlated Electrons · Physics 2020-10-01 E. C. Marino , Lizardo H. C. M. Nunes

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

In the framework of the Eupraxia Design Study an advanced accelerator facility EUPRAXIA@SPARC_LAB has been proposed to be realized at Frascati (Italy) Laboratories of INFN. Two advanced acceleration schemes will be applied, namely an…

CLIC is a proposed linear $e^+e^-$ collider with center-of-mass energies of up to 3 TeV. Its main objectives are precise top quark, Higgs boson and Beyond Standard Model physics. In addition to spatial resolutions of a few micrometers and a…

Instrumentation and Detectors · Physics 2021-03-10 Simon Spannagel
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