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Related papers: Physics aspects of polarized e+ at the linear coll…

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The physics case for electron-positron beams at the Future Circular Collider (FCC-ee) is succinctly summarized. The FCC-ee core program involves $e^+e^-$ collisions at $\sqrt{s}$ = 90, 160, 240, and 350 GeV with multi-ab$^{-1}$ integrated…

High Energy Physics - Experiment · Physics 2016-01-26 David d'Enterria

We consider the possibility of fingerprinting the presence of heavy additional Z' bosons that arise naturally in extensions of the standard model such as E_6 models and left-right symmetric models, through their mixing with the standard…

High Energy Physics - Phenomenology · Physics 2015-03-17 B. Ananthanarayan , Monalisa Patra , P. Poulose

Two next-generation high-energy experiments, the Large Hadron Collider (LHC) and the $e^+e^-$ International Linear Collider (ILC), are highly expected to unravel the new structure of matter and forces from the electroweak scale to the TeV…

High Energy Physics - Phenomenology · Physics 2007-11-15 S. Y. Choi

A polarized ep/eA collider (Electron-Ion Collider, or EIC) with variable center-of-mass energy sqrt(s) ~ 20-70 GeV and a luminosity ~ 10^{34} cm^{-2} s^{-1} would be uniquely suited to address several outstanding questions of Quantum…

Nuclear Theory · Physics 2015-05-30 A. Accardi , V. Guzey , A. Prokudin , C. Weiss

The International Linear Collider (ILC) is likely to provide us important insights into the sector of physics that may supersede our current paradigm viz., the Standard Model. In anticipation of the possibility that the ILC may come up in…

High Energy Physics - Phenomenology · Physics 2008-11-26 K. Sridhar

Electron-positron annihilation into a pair of top quarks is considered at the energy of the future collider CLIC. Polarization components of the top quark are calculated with the $\gamma t \bar{t}$ and $Z t \bar{t}$ interactions which…

High Energy Physics - Phenomenology · Physics 2019-05-28 I. V. Truten , A. Yu. Korchin

Linear collider designs are optimized for \ep\ collisions. However, from the physics point of view, \lc s may also be advantageously operated in an \ee, \eg\ or \pp\ mode. These options, which have not been available up to now, will provide…

High Energy Physics - Phenomenology · Physics 2007-05-23 Frank Cuypers , Geert Jan van Oldenborgh , Reinhold Rückl

If new particles are discovered, it will be important to determine if they are the supersymmetric partners of standard model bosons and fermions. Supersymmetry predicts relations among the couplings and masses of these particles. We discuss…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jonathan L. Feng

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 need to understand physics of electroweak symmetry breaking is reviewed. An electron positron linear collider will play crucial roles in that respect. It is discussed how the LHC and a linear collider need each other to understand…

High Energy Physics - Experiment · Physics 2007-05-23 Hitoshi Murayama

This letter reviews the potential of a high luminosity e+e- linear collider (LC) in the precision study of the Higgs boson profile. The complementarity with the Large Hadron Collider (LHC) Higgs physics program is briefly discussed.

High Energy Physics - Phenomenology · Physics 2007-05-23 Markus Schumacher

One of the most attractive features of a linear collider is the ability to extend its energy reach in stages, and to adapt the running plan flexibly in terms of maximum centre-of-mass energy and time spent at each stage. The baseline…

High Energy Physics - Experiment · Physics 2020-01-16 Aidan Robson , Philipp Roloff , Jorge de Blas

We utilize top polarization in the process e+ e-\rightarrow t\bar{t} at the ILC with transverse beam polarization to probe interactions of the scalar and tensor type beyond the standard model and to disentangle their individual…

High Energy Physics - Phenomenology · Physics 2011-02-01 B. Ananthanarayan , Monalisa Patra , Saurabh D. Rindani

In a series of notes we explore the detector requirements of the forward tracking region for a future $ e^+ e^- $ collider with a center-of-mass energy in the range from 500 GeV to 3 TeV. In this first part we investigate the relevance of…

High Energy Physics - Experiment · Physics 2010-01-11 J. Fuster , S. Heinemeyer , C. Lacasta , C. Marinas , A. Ruiz-Jimeno , M. Vos

We explore the usefulness of very energetic linear $e^+e^-$ colliders in the $TeV$ range in studying an alternative scheme of electroweak symmetry breaking based on a strong interacting sector. The calculations are performed within the BESS…

High Energy Physics - Phenomenology · Physics 2009-10-22 R. Casalbuoni , P. Chiappetta , A. Deandrea , S. De Curtis , D. Dominici , R. Gatto

Top quark production in the process $e^+e^- \rightarrow t\bar{t}$ at a future linear electron positron collider with polarized beams is a powerful tool to determine the scale of new physics. Studies at the $\ttbar$ threshold will allow for…

High Energy Physics - Experiment · Physics 2014-01-07 D. Asner , A. Hoang , Y. Kiyo , R. Pöschl , Y. Sumino , M. Vos

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

Some aspects of electroweak physics at the International Linear Collider (ILC) are reviewed. The importance of precision measurements in the Higgs sector and in top-quark physics is emphasized, and the physics potential of the GigaZ option…

High Energy Physics - Phenomenology · Physics 2008-11-26 Georg Weiglein

We study the sensitivity to the Z' couplings of the processes $e^+e^-\to l^+l^-,\bar{b}b$ and $\bar{c}c$ at the linear collider with $\sqrt{s}=500 GeV$ with initial beam polarization, for typical extended model examples. To this aim, we use…

High Energy Physics - Phenomenology · Physics 2011-01-25 A. A. Babich , A. A. Pankov , N. Paver

Linear colliders offer a unique possibility to study gamma gamma and gamma electron interactions at the energies 0.1--2 TeV. This option is now included in design reports of NLC, JLC and TESLA/SBLC. This paper includes: status of photon…

High Energy Physics - Experiment · Physics 2009-10-31 Valery Telnov