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Related papers: Positron Sources for Future High Energy Physics Co…

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Positron sources are the key elements for the future and current lepton collider projects such as ILC, CLIC, SuperKEKB, FCC-ee, Muon Collider/LEMMA, etc., introducing challenging critical requirements for high intensity and low emittance…

The high-luminosity requirement in future lepton colliders imposes a need for a high-intensity positron source. In the conventional scheme, positron beams are obtained by the conversion of bremsstrahlung photons into electron-positron pairs…

In order to achieve the physics goals of future Linear Colliders, it is important that electron and positron beams are polarized. The baseline design at the International Linear Collider (ILC) foresees an e+ source based on helical…

Accelerator Physics · Physics 2012-02-06 V. Kovalenko , O. S. Adeyemi , A. Hartin , G. Moortgat-Pick , L. Malysheva , S. Riemann , F. Staufenbiel , A. Ushakov

The design of the positron source for the International Linear Collider (ILC) is still under discussion. The baseline design plans to use the high-energy electron beam for the positron production before it goes to the IP. The electrons pass…

Accelerator Physics · Physics 2020-02-26 Sabine Riemann , Peter Sievers , Gudrid Moortgat-Pick , Andriy Ushakov

Several designs for high-energy Lepton Colliders serving as Higgs factories but extendable to higher energies up to the TeV range are under discussion. The most mature design is the International Linear Collider (ILC), but also the Compact…

High Energy Physics - Phenomenology · Physics 2023-09-28 Gudrid Moortgat-Pick , Sabine Riemann , Peter Sievers , Carmen Tenholt

High energy e+e- linear colliders are the next large scale project in particle physics. They need intense sources to achieve the required luminosity. In particular, the positron source must provide about 10E+14 positrons per second. The…

Accelerator Physics · Physics 2014-12-11 S. Riemann , F. Staufenbiel , G. Moortgat-Pick , A. Ushakov

Recent advances in electron and positron sources have resulted in new capabilities driven in most cases by the increasing demands of advanced accelerating systems. Electron sources for brighter beams and for high average-current beams are…

Accelerator Physics · Physics 2009-11-06 J. E. Clendenin

The design of the positron source for the International Linear Collider (ILC) is still under consideration. The baseline design plans to use the electron beam for the positron production before it goes to the IP. The high-energy electrons…

Accelerator Physics · Physics 2019-02-22 Felix Dietrich , Gudrid Moortgat-Pick , Sabine Riemann , Peter Sievers , Andriy Ushakov

The full exploitation of the physics potential of an International Linear Collider (ILC) requires the development of a polarized positron beam. New concepts of polarized positron sources are based on the development of circularly polarized…

Instrumentation and Detectors · Physics 2009-11-11 Ralph Dollan , Karim Laihem , Andreas Schaelicke

For the planned International Linear Collider it is intended to have both -- electron and positron -- beams polarised. This offers a great benefit for many physics studies, but also provides a challenge for the engineering of the machine. A…

High Energy Physics - Experiment · Physics 2008-11-26 Andreas Schälicke

Various methods of obtaining longitudinally polarized positrons for future linear colliders are reviewed. Special attention is paid to the schemes using circularly polarized high-energy photons for positron production. Most effectively such…

High Energy Physics - Phenomenology · Physics 2009-11-10 V. Strakhovenko , X. Artru , R. Chehab , M. Chevallier

Future electron-positron linear colliders require a highly polarized electron beam with a pulse structure that depends primarily on whether the acceleration utilizes warm or superconducting rf structures. The International Linear Collider…

Beam polarisation is an integral part of the physics case of future Linear Colliders. In this contribution, important examples from Higgs coupling measurements, top and electroweak physics at high energies, the Z pole program as well as…

High Energy Physics - Experiment · Physics 2021-02-10 Jenny List

Plasma based acceleration is considered a promising concept for the next generation of linear electron-positron colliders. Despite the great progress achieved over last twenty years in laser technology, laser and beam driven particle…

Plasma Physics · Physics 2023-11-21 S. S. Bulanov , C. Benedetti , D. Terzani , C. B. Schroeder , E. Esarey , T. Blackburn , M. Marklund

A short overview about the potential of polarized beams at future colliders is given. In particular the baseline design for polarized beams at the ILC is presented and the physics case for polarized $e^-$ and $e^+$ is discussed. In order to…

This document presents an overview of the physics potential of a future electron-positron linear collider. It represents a common input from the CLIC and ILC communities.

In this paper we review the physics opportunities at linear $e^+e^-$ colliders with a special focus on high centre-of-mass energies and beam polarisation, take a fresh look at the various accelerator technologies available or under…

High Energy Physics - Experiment · Physics 2025-12-24 H. Abramowicz , E. Adli , F. Alharthi , M. Almanza-Soto , M. M. Altakach , W. Altmannshofer , S. Ampudia Castelazo , D. Angal-Kalinin , J. A. Anguiano , R. B. Appleby , O. Apsimon , A. Arbey , F. Arco , O. Arquero , A. Aryshev , S. Asai , D. Attie , J. L. Avila-Jimenez , H. Baer , J. A. Bagger , Y. Bai , I. R. Bailey , C. Balazs , P. Bambade , T. Barklow , J. Baudot , P. Bechtle , T. Behnke , A. B. Bellerive , S. Belomestnykh , Y. Benhammou , J. Berenguer-Antequera , M. Berger , M. Berggren , M. Bertucci , M. Besancon , D. Bett , P. -C. Bhat , T. Biekoetter , S. Bilanishvili , B. Bilki , B. Bilki , J. Bjorklund Svensson , V. M. Bjelland , C. Blanch , B. Bliewert , M. Boehler , S. Boogert , M. Boronat , V. Boudry , D. Bourilkov , I. Bozovic , J. Braathen , J. E. Brau , C. Breuning , J. -C. Brient , I. Brock , B. Brudnowski , K. Buesser , E. Bulyak , P. N. Burrows , G. Burt , O. Cakir , A. Caldwell , A. C. Canbay , F. G. Celiberto , E. Cenni , I. Chaikovska , R. Chehab , G. Chen , J. B. B. Chen , T. Chikamatsu , V. Cilento , P. Colas , M. Coman , L. Corner , F. Cornet , F. Cornet-Gomez , F. Corriveau , R. Corsini , J. Cvach , R. D'Arcy , C. Damerell , A. Das , S. Dasu , J. de Blas , E. Del Core , M. Demarteau , H. Denizli , R. Dermisek , A. Dhar , S. Dittmaier , F. Djurabekova , E. M. Donegani , A. Doyle , P. Drobniak , T. A. du Pree , B. Dudar , H. Duran Yildiz , G. Durieux , J. Dutta , S. Easo , G. Eckerlin , U. Einhaus , C. Emma , E. Esarey , D. Esperante , D. Espriu , L. R Evans , J. Farmer , A. Faus Golfe , M. Fernandez , J. C. Fernandez-Ortega , M. Formela , A. Formenti , L. J. Forrester , B. Foster , N. Fourches , M. C. Fouz , A. Freitas , C. D. Fu , K. Fujii , J. Fujimoto , B. Fuks , J. Fuster , N. Fuster-Martinez , M. Gabelmann , F. Gaede , M. Galletti , E. Gallo , S. Ganjour , M. V. Garzelli , R. L. Geng , S. Gessner , I. D. Gialamas , B. Gimeno , J. Goldstein , M. Goncerz , A. J. Gonsalves , F. J. Gonzalez , D. Gonzalez-Iglesias , S. Gori , J. Grames , P. Grannis , L. Gray , G. Grenier , H. Guler , H. E. Haber , K. Hamaguchi , N. Hamann , O. Hartbrich , N. M. Hartman , G. Huetsi , S. Heinemeyer , G. Heinrich , C. Hensel , K. Hidaka , S. Hirose , A. H. Hoang , M. J. Hogan , W. Hollik , Y. Horii , R. Hosokawa , S. Huang , D. Hynds , M. I. Idzik , S. Iguro , Y. Iiyama , K. Ikematsu , A. Irles , A. Ishikawa , M. Ishino , I. P. Ivanov , Y. Iwashita , M. Jacewicz , R. Jaramillo , D. Jeans , C. Jing , R. M Jones , W. Kaabi , M. Kagan , J. Kalinowski , D. K Kalvik , J. Kaminski , S. Kanemura , K. Kannike , A. Karam , Y. Kato , K. Kawagoe , D. Kaefer , L. Kennedy , J. Kersten , S. A. Khan , V. A. Khoze , W. Kilian , J. Klamka , P. Kluit , K. Kong , P. Koppenburg , A. Korsun , A. V. Kotwal , S. Kraml , K. Krueger , K. Kubo , T. Kubo , M. Kucharczyk , S. Kuday , A. Kumar , N. Kumar , M. Kurata , Y. Kurihara , M. Kuriki , J. Kvasnicka , K. Kyoya , I. Laktineh , A. Latina , F. LeDiberder , A. Levy , M. Liepe , C. A. Lindstroem , J. List , B. List , M. Litos , V. N. Litvinenko , A. Lopez-Virto , X. Lu , T. Luo , M. Lupberger , B. Madison , T. Madlener , J. Maeda , F. Mahmoudi , E. Maina , N. Majernik , R. Margraf-O'Neal , T. W. Markiewicz , P. Martin-Luna , A. Martens , V. J. Martin , L. Marzola , V. I. Maslov , K. T. Matchev , S. Matsumoto , K. Mawatari , J. P. Marquez , M. M. Muehlleitner , A. McIlvenny , P. A. McIntosh , K. Mekala , D. Melini , F. Meloni , A. Menandez , S. Michizono , K. Mimasu , V. Miralles , W. Mitaroff , V. A. Mitsou , L. Monaco , G. Moortgat-Pick , M. Moreno-Llcer , T. Mori , J. M. Moron , S. Morton , D. Moya , M. Mulder , P. Munbodh , H. Murayama , E. Musumeci , V. V. Mytrochenko , N. Nagata , E. Nagy , T. Nakada , J. Nakajima , K. Nakamura , E. A. Nanni , E. Nardi , S. Narita , M. T. Nunez Pardo de Vera , M. Nojiri , D. Ntounis , A. Ody , O. M. Ogreid , T. Ohl , Y. Okada , C. Oleari , M. Olvegard , M. Omet , T. Omori , Y. Onel , H. Ono , W. Ootani , C. Orero , J. Osborne , K. Osterberg , J. Osterhoff , M. Ouchemhou , Q. Ouyang , S. Pagan Griso , R. Paparella , S. C. Park , J. Pata , J. R. Patterson , R. Poeschl , F. Pena , L. K Pedraza-Motavita , M. E. Peskin , F. Pilat , P. Piot , S. Plaetzer , I. Polak , W. Porod , K. Potamianos , C. T. Potter , P. Poulose , J. G. Power , D. Protopopescu , H. R. Qi , J. Rabara Bailey , A. Racioppi , M. Raidal , J. P. Ralston , A. Rastogi , L. Reichenbach , L. Reichwein , L. Reina , J. Reuter , F. Richard , S. Riemann , R. A. Rimmer , T. Robens , A. Robson , G. Rodrigo , C. S. Rogan , J. Rojo , M. Q. Ruan , S. Rudrabhatla , A. Ruiz Jimeno , T. Saeki , H. Sakai , Y. Sakaki , F. Salvatore , T. Sanuki , S. Sasikumar , T Schoerner , A. Scheinker , C. B. Schroeder , S. Schroeder , I. Schulthess , M. Schumacher , A. Schwartzman , Y. Seiya , A. Senol , H. Sert , D. Sertore , A. Seryi , T. Shidara , K. Sjobak , I. Smiljanic , S. Spannagel , M. Spira , M. Stanitzki , S. Stapnes , D. Storey , J. Strube , S. Su , A. Subba , A. Subba , T. Suehara , H. Sugawara , K. Sugizaki , Z. Sun , R. Szafron , T. Takahashi , T. Takeshita , T. Tauchi , G. Taylor , N. Terunuma , D. Terzani , T. Teubner , J. Tian , J. Timmermans , M. Titov , R. Tomas Garcia , T. Tong , J. M. Torndal , M. Trautwein , A. Tricoli , K. Tsumura , B. Tuchming , D. Tuckler , I. Turk Cakir , M. Tytgat , A. Ukleja , C. Vallee , R. Van Kooten , J. van Tilborg , A. Vauth , M. Vellasco , C. Vernieri , L. Verra , M. Vicente Barreto Pinto , I. Vidakovic , H. Videau , E. Viklund , I. Vila , M. Villaplana , M. Vos , N. Vukasinovic , N. Walker , K. Wandall-Christensen , Y. Wang , B. F. L. Ward , Z. Was , T. Watanabe , N. K. Watson , G. Weiglein , J. D. Wells , H. Wennloef , M. Wenskat , S. Westhoff , J. W. Wetzel , A. P. White , P. H. Williams , M. Williams , G. W. Wilson , M. Wing , M. Winter , A. Winter , T. Wojton , J. C. Wood , W. Wuensch , X. Xia , K. Yagyu , K. Yamamoto , Y. Yamamoto , H. Yamamoto , A. Yamamoto , S. Yamashita , M. Yamauchi , K. Yokoya , M. Yoshioka , J. Zalesak , A. F. Zarnecki , K. Zembaczynski , D. Zerwas , J. Zhang , Y. Zhang , W. Zhang , Y. -M. Zhong , M. Zielinski , M. Zobov

Compact spin-polarized positron accelerators play a major role in promoting significant positron application research, which typically require high acceleration gradients and polarization degree, both of which, however, are still great…

Plasma Physics · Physics 2024-05-21 Zhen-Ke Dou , Chong Lv , Yousef I. Salamin , Nan Zhang , Feng Wan , Zhong-Feng Xu , Jian-Xing Li

The full exploitation of the physics potential of a future Linear Collider requires the development of polarised positron beams. A very promising scheme for the technical realisation is the use of helical undulators, generating circular…

High Energy Physics - Phenomenology · Physics 2011-09-13 Gudrid Moortgat-Pick

In the baseline design of the International Linear Collider (ILC) an undulator-based source is foreseen for the positron source in order to match the physics requirements. The recently chosen first energy stage with sqrt(s)=250 GeV requires…

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