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Related papers: Beam dynamics and wake-field simulations for the C…

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We quantify the discovery potential of future multi-TeV plasma wakefield colliders for new electroweak multiplets. We include beam-beam effects through realistic luminosity spectra, comparing five collider configurations: $e^+e^-$ and…

High Energy Physics - Phenomenology · Physics 2025-12-12 So Chigusa , Simon Knapen , Toby Opferkuch , Inbar Savoray , Christiane Scherb , Weishuang Linda Xu

Recent experiments at SLAC [1,2] and CERN [3] have revealed evidence of significant deformation in the form of "pitting" of the cells of the 1.8m series of structures DDS/RDDS (Damped Detuned Structure/Rounded Damped Detuned Structure).…

Accelerator Physics · Physics 2008-11-26 R. M. Jones , N. M. Kroll , T. Higo , Z. Li , R. H. Miller , T. O. Raubenheimer , J. W. Wang

Interest in highly-compressed electron beams has been increasing in recent times, driven by the study of non-linear and even non-perturbative aspects of QED [2]. The FACET-II [7] facility at SLAC is currently (at the time of writing) being…

Accelerator Physics · Physics 2018-11-30 Glen White , Vitaly Yakimenko

It is proposed to place the arcs of an SLC-type facility inside the tunnel of a Future Circular Collider (FCC). Accelerated by a linear accelerator (linac), electron and positron beams would traverse the bending arcs in opposite directions…

Accelerator Physics · Physics 2018-06-28 Radoje Belusevic

The post-linac energy collimation system of multi-TeV linear colliders is designed to fulfil an important function of protection of the Beam Delivery System (BDS) against miss-steered beams likely generated by failure modes in the main…

Accelerator Physics · Physics 2011-12-22 Javier Resta-Lopez

Though wakefield acceleration in crystal channels has been previously proposed, x-ray wakefield acceleration has only recently become a realistic possibility since the invention of the single-cycled optical laser compression technique. We…

Collinear high-gradient ${\cal O} (GV/m)$ beam-driven wakefield methods for charged-particle acceleration could be critical to the realization of compact, cost-efficient, accelerators, e.g., in support of TeV-scale lepton colliders or…

Accelerator Physics · Physics 2015-09-30 Francois Lemery , Philippe Piot

The JAERI/KEK Joint Project for the high-intensity proton accelerator facility has been proposed with a superconducting (SC) linac option from 400 MeV to 600MeV. System design of the SC linac has been carried out based on the…

The Compact Linear Collider (CLIC) is a proposed future high-luminosity linear electron-positron collider operating at three energy stages, with nominal centre-of-mass energies: 380 GeV, 1.5 TeV, and 3 TeV. Its aim is to explore the energy…

High Energy Physics - Experiment · Physics 2019-11-21 H. Abramowicz , N. Alipour Tehrani , D. Arominski , Y. Benhammou , M. Benoit , J. -J. Blaising , M. Boronat , O. Borysov , R. R. Bosley , I. Božović Jelisavčić , I. Boyko , S. Brass , E. Brondolin , P. Bruckman de Renstrom , M. Buckland , P. N. Burrows , M. Chefdeville , S. Chekanov , T. Coates , D. Dannheim , M. Demarteau , H. Denizli , G. Durieux , G. Eigen , K. Elsener , E. Fullana , J. Fuster , M. Gabriel , F. Gaede , I. García , J. Goldstein , P. Gomis Lopez , C. Graf , S. Green , C. Grefe , C. Grojean , A. Hoang , D. Hynds , A. Joffe , J. Kalinowski , G. Kačarević , W. Kilian , N. van der Kolk , M. Krawczyk , M. Kucharczyk , E. Leogrande , T. Lesiak , A. Levy , I. Levy , L. Linssen , A. A. Maier , V. Makarenko , J. S. Marshall , V. Martin , V. Mateu , O. Matsedonskyi , J. Metcalfe , G. Milutinović Dumbelović , R. M. Münker , Yu. Nefedov , K. Nowak , A. Nürnberg , M. Pandurović , M. Perelló , E. Perez Codina , M. Petric , F. Pitters , T. Price , T. Quast , S. Redford , J. Repond , A. Robson , P. Roloff , E. Ros , K. Rozwadowska , A. Ruiz-Jimeno , A. Sailer , F. Salvatore , U. Schnoor , D. Schulte , A. Senol , G. Shelkov , E. Sicking , F. Simon , R. Simoniello , P. Sopicki , S. Spannagel , S. Stapnes , R. Ström , M. Szalay , M. A. Thomson , B. Turbiarz , O. Viazlo , M. Vicente , I. Vila , M. Vos , J. Vossebeld , M. F. Watson , N. K. Watson , M. A. Weber , H. Weerts , J. D. Wells , A. Widl , M. Williams , A. G. Winter , T. Wojtoń , A. Wulzer , B. Xu , L. Xia , T. You , A. F. Żarnecki , L. Zawiejski , C. Zhang , J. Zhang , Y. Zhang , Z. Zhang , A. Zhemchugov

Early tests of short low group velocity and standing wave structures indicated the viability of operating X-band linacs with accelerating gradients in excess of 100 MeV/m. Conventional scaling of traveling wave traveling wave linacs with…

This paper describes simulation analyses on beam and laser (X-ray)-driven accelerations in effective nanotube models obtained from Vsim and EPOCH codes. Experimental setups to detect wakefields are also outlined with accelerator facilities…

Interaction between the bunches in the NLC main linac via long range wakefields can cause a beam breakup instability. Although the magnitude of the long range wakefields for an ideal NLC structure is below the instability threshold, the…

Accelerator Physics · Physics 2007-05-23 G. V. Stupakov

Longitudinal space charge (LSC) effects are generally considered harmful in free-electron lasers as they can seed unfavorable energy modulations that can result in density modulations with associated emittance dilution. It was pointed out,…

Accelerator Physics · Physics 2016-07-28 A. Halavanau , P. Piot

Linear accelerators containing the sequence of independently phased cavities with constant geometrical velocity along each structure are widely used in practice. The chain of cavities with identical cell lengths is utilized within a certain…

Accelerator Physics · Physics 2023-02-21 Yuri K. Batygin

A high peak current, flat longitudinal phase space electron beam is desirable for efficient x-ray free electron laser (FEL) radiation in next generation light sources. To attain such a beam requires the extensive design of the linear…

Accelerator Physics · Physics 2019-10-23 Ji Qiang

The energy spread in laser-wakefield accelerators is primarily limited by the energy-chirp introduced during the injection and acceleration processes. Here we propose and demonstrate the use of longitudinal density tailoring to adapt the…

Accelerator Physics · Physics 2018-08-22 A. Döpp , C. Thaury , E. Guillaume , F. Massimo , A. Lifschitz , I. Andriyash , J. -P. Goddet , A. Tazfi , K. Ta Phuoc , V. Malka

One of the main concerns in the design of low emittance linear accelerators (linacs) is the preservation of beam emittance. Here we discuss one possible source of emittance dilution, the coupler kick, due to transverse electromagnetic…

Accelerator Physics · Physics 2008-11-26 Brandon Buckley , Georg H. Hoffstaetter

The Linear Accelerator 4 (LINAC 4) is designed to accelerate negative hydrogen ions to high energies for injection into the Large Hadron Collider (LHC), where it has been supplying proton beams since 2020. LINAC 4 accelerates negative…

Accelerator Physics · Physics 2025-03-04 D. M. C. M. K. Dissanayake , N. Wickramage , K. M. Liyanage , K. A. S. Lakshan

Reducing the operating temperature of normal conducting particle accelerators substantially increases their efficiency. Low-temperature operation increases the yield strength of the accelerator material and reduces surface resistance, hence…

Accelerator Physics · Physics 2021-09-22 Mamdouh Nasr , Emilio Nanni , Martin Breidenbach , Stephen Weathersby , Marco Oriunno , Sami Tantawi

The beam-beam interaction is one of the dominant sources of emittance growth and luminosity lifetime deterioration. A current carrying wire has been proposed to compensate long-range beam-beam effects in the LHC and strong localized…

Accelerator Physics · Physics 2011-04-12 Hyung J. Kim , Tanaji Sen , Natalia P. Abreu , Wolfram Fischer
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