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Compensation of multi-bunch beam loading is of great importance in the main linac of the Compact Linear Collider (CLIC). The bunch-to-bunch energy variation has to stay below 1 part in 1000. In CLIC, the RF power is obtained by decelerating…

Accelerator Physics · Physics 2007-05-23 D. Schulte , I. Syratchev

As a charged particle beam moves through perfectly conducting structures with varying cross-sectional boundaries - such as RF cavities, tapers, bellows, kickers, ... - it induces both longitudinal and transverse electromagnetic fields…

Accelerator Physics · Physics 2025-05-21 Massimo Ferrario , Mauro Migliorati , Luigi Palumbo

When a charged particle travels across the vacuum chamber of an accelerator, it induces electromagnetic fields, which are left mainly behind the generating particle. These electromagnetic fields act back on the beam and influence its…

Accelerator Physics · Physics 2016-01-21 M. Ferrario , M. Migliorati , L. Palumbo

Three-dimensional Particle-in-Cell (PIC) simulations with the code QuickPIC are used to illustrate the typical accelerating structures associated with the interaction of an intense laser beam with an underdense plasma in the blowout regime.…

The Compact Linear Collider (CLIC) is a proposed high-luminosity linear electron-positron collider at the energy frontier. It is foreseen to be built and operated in three stages, with a centre-of-mass energy ranging from a few hundred GeV…

High Energy Physics - Experiment · Physics 2018-11-02 Erica Brondolin , Andre Sailer

CLIC is a linear $e^+e^-$ ($\gamma\gamma$) collider project which uses a drive beam to accelerate the main beam. The drive beam provides RF power for each corresponding unit of the main linac through energy extracting RF structures. CLIC…

Accelerator Physics · Physics 2007-05-23 Husnu Aksakal

Important efforts have recently been dedicated to the characterisation and improvement of the design of the post-linac collimation system of the Compact Linear Collider (CLIC). This system consists of two sections: one dedicated to the…

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

In order to dissipate long-lived radioactive waste, not only high ux proton accelerator but also electron linac have been proposed. A proton accelerator directly induces nuclear fission and mutation. On the other hand, electron beam has two…

Accelerator Physics · Physics 2021-04-20 Y. Kawashima , T. Asaka , H. Ego , M. Hara

The Compact Linear Collider CLIC is designed to deliver e+e- collisions at a center of mass energy of up to 3 TeV. The detector systems at this collider have to provide highly efficient tracking and excellent jet energy resolution and…

Instrumentation and Detectors · Physics 2011-09-16 Frank Simon

A crab cavity is required in the CLIC to allow effective head-on collision of bunches at the IP. A high operating frequency is preferred as the deflection voltage required for a given rotation angle and the RF phase tolerance for a crab…

Accelerator Physics · Physics 2009-06-22 P. K. Ambattu , G. Burt , A. C. Dexter , R. G. Carter , V. Khan , R. M. Jones , V. Dolgashev

Metre-scale plasma wakefield accelerators have imparted energy gain approaching 10 gigaelectronvolts to single nano-Coulomb electron bunches. To reach useful average currents, however, the enormous energy density that the driver deposits…

The Compact Linear Collider (CLIC) is a proposed high-luminosity collider that would collide electrons with their antiparticles, positrons, at energies ranging from a few hundred Giga-electronvolts (GeV) to a few Tera-electronvolts (TeV).…

Accelerator Physics · Physics 2020-04-22 Eva Sicking , Rickard Ström

The Compact Linear Collider (CLIC) is a multi-TeV high-luminosity linear e+e- collider under development. For an optimal exploitation of its physics potential, CLIC is foreseen to be built and operated in a staged approach with three…

Accelerator Physics · Physics 2017-03-28 The CLIC , CLICdp collaborations , : , M. J. Boland , U. Felzmann , P. J. Giansiracusa , T. G. Lucas , R. P. Rassool , C. Balazs , T. K. Charles , K. Afanaciev , I. Emeliantchik , A. Ignatenko , V. Makarenko , N. Shumeiko , A. Patapenka , I. Zhuk , A. C. Abusleme Hoffman , M. A. Diaz Gutierrez , M. Vogel Gonzalez , Y. Chi , X. He , G. Pei , S. Pei , G. Shu , X. Wang , J. Zhang , F. Zhao , Z. Zhou , H. Chen , Y. Gao , W. Huang , Y. P. Kuang , B. Li , Y. Li , J. Shao , J. Shi , C. Tang , X. Wu , L. Ma , Y. Han , W. Fang , Q. Gu , D. Huang , X. Huang , J. Tan , Z. Wang , Z. Zhao , T. Laštovička , U. Uggerhoj , T. N. Wistisen , A. Aabloo , K. Eimre , K. Kuppart , S. Vigonski , V. Zadin , M. Aicheler , E. Baibuz , E. Brücken , F. Djurabekova , P. Eerola , F. Garcia , E. Haeggström , K. Huitu , V. Jansson , V. Karimaki , I. Kassamakov , A. Kyritsakis , S. Lehti , A. Meriläinen , R. Montonen , T. Niinikoski , K. Nordlund , K. Österberg , M. Parekh , N. A. Törnqvist , J. Väinölä , M. Veske , W. Farabolini , A. Mollard , O. Napoly , F. Peauger , J. Plouin , P. Bambade , I. Chaikovska , R. Chehab , M. Davier , W. Kaabi , E. Kou , F. LeDiberder , R. Pöschl , D. Zerwas , B. Aimard , G. Balik , J. -P. Baud , J. -J. Blaising , L. Brunetti , M. Chefdeville , C. Drancourt , N. Geoffroy , J. Jacquemier , A. Jeremie , Y. Karyotakis , J. M. Nappa , S. Vilalte , G. Vouters , A. Bernard , I. Peric , M. Gabriel , F. Simon , M. Szalay , N. van der Kolk , T. Alexopoulos , E. N. Gazis , N. Gazis , E. Ikarios , V. Kostopoulos , S. Kourkoulis , P. D. Gupta , P. Shrivastava , H. Arfaei , M. K. Dayyani , H. Ghasem , S. S. Hajari , H. Shaker , Y. Ashkenazy , H. Abramowicz , Y. Benhammou , O. Borysov , S. Kananov , A. Levy , I. Levy , O. Rosenblat , G. D'Auria , S. Di Mitri , T. Abe , A. Aryshev , T. Higo , Y. Makida , S. Matsumoto , T. Shidara , T. Takatomi , Y. Takubo , T. Tauchi , N. Toge , K. Ueno , J. Urakawa , A. Yamamoto , M. Yamanaka , R. Raboanary , R. Hart , H. van der Graaf , G. Eigen , J. Zalieckas , E. Adli , R. Lillestøl , L. Malina , J. Pfingstner , K. N. Sjobak , W. Ahmed , M. I. Asghar , H. Hoorani , S. Bugiel , R. Dasgupta , M. Firlej , T. A. Fiutowski , M. Idzik , M. Kopec , M. Kuczynska , J. Moron , K. P. Swientek , W. Daniluk , B. Krupa , M. Kucharczyk , T. Lesiak , A. Moszczynski , B. Pawlik , P. Sopicki , T. Wojtoń , L. Zawiejski , J. Kalinowski , M. Krawczyk , A. F. Żarnecki , E. Firu , V. Ghenescu , A. T. Neagu , T. Preda , I-S. Zgura , A. Aloev , N. Azaryan , J. Budagov , M. Chizhov , M. Filippova , V. Glagolev , A. Gongadze , S. Grigoryan , D. Gudkov , V. Karjavine , M. Lyablin , A. Olyunin , A. Samochkine , A. Sapronov , G. Shirkov , V. Soldatov , A. Solodko , E. Solodko , G. Trubnikov , I. Tyapkin , V. Uzhinsky , A. Vorozhtov , E. Levichev , N. Mezentsev , P. Piminov , D. Shatilov , P. Vobly , K. Zolotarev , I. Bozovic Jelisavcic , G. Kacarevic , S. Lukic , G. Milutinovic-Dumbelovic , M. Pandurovic , U. Iriso , F. Perez , M. Pont , J. Trenado , M. Aguilar-Benitez , J. Calero , L. Garcia-Tabares , D. Gavela , J. L. Gutierrez , D. Lopez , F. Toral , D. Moya , A. Ruiz Jimeno , I. Vila , T. Argyropoulos , C. Blanch Gutierrez , M. Boronat , D. Esperante , A. Faus-Golfe , J. Fuster , N. Fuster Martinez , N. Galindo Muñoz , I. García , J. Giner Navarro , E. Ros , M. Vos , R. Brenner , T. Ekelöf , M. Jacewicz , J. Ögren , M. Olvegård , R. Ruber , V. Ziemann , D. Aguglia , N. Alipour Tehrani , A. Andersson , F. Andrianala , F. Antoniou , K. Artoos , S. Atieh , R. Ballabriga Sune , M. J. Barnes , J. Barranco Garcia , H. Bartosik , C. Belver-Aguilar , A. Benot Morell , D. R. Bett , S. Bettoni , G. Blanchot , O. Blanco Garcia , X. A. Bonnin , O. Brunner , H. Burkhardt , S. Calatroni , M. Campbell , N. Catalan Lasheras , M. Cerqueira Bastos , A. Cherif , E. Chevallay , B. Constance , R. Corsini , B. Cure , S. Curt , B. Dalena , D. Dannheim , G. De Michele , L. De Oliveira , N. Deelen , J. P. Delahaye , T. Dobers , S. Doebert , M. Draper , F. Duarte Ramos , A. Dubrovskiy , K. Elsener , J. Esberg , M. Esposito , V. Fedosseev , P. Ferracin , A. Fiergolski , K. Foraz , A. Fowler , F. Friebel , J-F. Fuchs , C. A. Fuentes Rojas , A. Gaddi , L. Garcia Fajardo , H. Garcia Morales , C. Garion , L. Gatignon , J-C. Gayde , H. Gerwig , A. N. Goldblatt , C. Grefe , A. Grudiev , F. G. Guillot-Vignot , M. L. Gutt-Mostowy , M. Hauschild , C. Hessler , J. K. Holma , E. Holzer , M. Hourican , D. Hynds , Y. Inntjore Levinsen , B. Jeanneret , E. Jensen , M. Jonker , M. Kastriotou , J. M. K. Kemppinen , R. B. Kieffer , W. Klempt , O. Kononenko , A. Korsback , E. Koukovini Platia , J. W. Kovermann , C-I. Kozsar , I. Kremastiotis , S. Kulis , A. Latina , F. Leaux , P. Lebrun , T. Lefevre , L. Linssen , X. Llopart Cudie , A. A. Maier , H. Mainaud Durand , E. Manosperti , C. Marelli , E. Marin Lacoma , R. Martin , S. Mazzoni , G. Mcmonagle , O. Mete , L. M. Mether , M. Modena , R. M. Münker , T. Muranaka , E. Nebot Del Busto , N. Nikiforou , D. Nisbet , J-M. Nonglaton , F. X. Nuiry , A. Nürnberg , M. Olvegard , J. Osborne , S. Papadopoulou , Y. Papaphilippou , A. Passarelli , M. Patecki , L. Pazdera , D. Pellegrini , K. Pepitone , E. Perez Codina , A. Perez Fontenla , T. H. B. Persson , M. Petrič , F. Pitters , S. Pittet , F. Plassard , R. Rajamak , S. Redford , Y. Renier , S. F. Rey , G. Riddone , L. Rinolfi , E. Rodriguez Castro , P. Roloff , C. Rossi , V. Rude , G. Rumolo , A. Sailer , E. Santin , D. Schlatter , H. Schmickler , D. Schulte , N. Shipman , E. Sicking , R. Simoniello , P. K. Skowronski , P. Sobrino Mompean , L. Soby , M. P. Sosin , S. Sroka , S. Stapnes , G. Sterbini , R. Ström , I. Syratchev , F. Tecker , P. A. Thonet , L. Timeo , H. Timko , R. Tomas Garcia , P. Valerio , A. L. Vamvakas , A. Vivoli , M. A. Weber , R. Wegner , M. Wendt , B. Woolley , W. Wuensch , J. Uythoven , H. Zha , P. Zisopoulos , M. Benoit , M. Vicente Barreto Pinto , M. Bopp , H. H. Braun , M. Csatari Divall , M. Dehler , T. Garvey , J. Y. Raguin , L. Rivkin , R. Zennaro , A. Aksoy , Z. Nergiz , E. Pilicer , I. Tapan , O. Yavas , V. Baturin , R. Kholodov , S. Lebedynskyi , V. Miroshnichenko , S. Mordyk , I. Profatilova , V. Storizhko , N. Watson , A. Winter , J. Goldstein , S. Green , J. S. Marshall , M. A. Thomson , B. Xu , W. A. Gillespie , R. Pan , M. A Tyrk , D. Protopopescu , A. Robson , R. Apsimon , I. Bailey , G. Burt , D. Constable , A. Dexter , S. Karimian , C. Lingwood , M. D. Buckland , G. Casse , J. Vossebeld , A. Bosco , P. Karataev , K. Kruchinin , K. Lekomtsev , L. Nevay , J. Snuverink , E. Yamakawa , V. Boisvert , S. Boogert , G. Boorman , S. Gibson , A. Lyapin , W. Shields , P. Teixeira-Dias , S. West , R. Jones , N. Joshi , R. Bodenstein , P. N. Burrows , G. B. Christian , D. Gamba , C. Perry , J. Roberts , J. A. Clarke , N. A. Collomb , S. P. Jamison , B. J. A. Shepherd , D. Walsh , M. Demarteau , J. Repond , H. Weerts , L. Xia , J. D. Wells , C. Adolphsen , T. Barklow , M. Breidenbach , N. Graf , J. Hewett , T. Markiewicz , D. McCormick , K. Moffeit , Y. Nosochkov , M. Oriunno , N. Phinney , T. Rizzo , S. Tantawi , F. Wang , J. Wang , G. White , M. Woodley

The Compact Linear Collider (CLIC) is a TeV-scale high-luminosity linear e$^+$e$^-$ collider studied by the international CLIC and CLICdp collaborations. CLIC uses a two-beam acceleration scheme, in which normal-conducting high-gradient 12…

The dense beams used at CLIC to achieve a high luminosity will cause a large amount of background particles through beam-beam interactions. Generator level studies with GuineaPig and full detector simulation studies with an ILD based CLIC…

Instrumentation and Detectors · Physics 2010-06-18 André Sailer

During the course of the last decade, traveling wave accelerating structures for a future Linear Collider have been the object of intense R&D efforts. An important problem is the efficient computation of the long range wakefield with the…

Accelerator Physics · Physics 2008-11-26 J. -F. Ostiguy , K. -Y. Ng

CLIC is a proposed linear $e^{+}e^{-}$ collider with center-of-mass energies of up to $3\,\textrm{TeV}$. Its main objectives are precise top quark and Higgs boson measurements, as well as searches for Beyond Standard Model physics. To meet…

Instrumentation and Detectors · Physics 2018-12-07 Simon Spannagel

The demands on performance of advanced linear accelerator based facilities strongly depend on the quality of the particle beams produced by such machines. Indeed, state-of-the-art applications in photon production and high-energy physics…

Operating the SLAC/KEK DDS (Damped Detuned Structure) X-band linacs at high gradients (in excess of 70MV/m) has recently been found to be limited by the accelerator structures breaking down and as a consequence severe damage occurs to the…

Accelerator Physics · Physics 2008-11-26 R. M. Jones , N. M. Kroll , T. Higo , R. H. Miller , R. D Ruth