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The International Linear Collider and other proposed high energy e+ e- machines aim to measure with unprecedented precision Standard Model quantities and new, not yet discovered phenomena. One of the main requirements for achieving this…

The rapid increase of the e+e- --> W+W- cross section in the threshold region provides a method for measuring M(W) at LEP2. The dependence of the theoretical cross section -- including the effects of the finite W width, Coulomb interactions…

High Energy Physics - Phenomenology · Physics 2016-09-01 W. J. Stirling

The expected experimental precision of the rates and asymmetries in the Future Circular Collider with electron positron beams (FCC-ee) in the centre of the mass energy range 88-365GeV considered for construction in CERN, will be better by a…

High Energy Physics - Phenomenology · Physics 2019-11-22 S. Jadach , M. Skrzypek

We report on the commissioning of a fast electron-energy scan system for measurements of electron-impact ionization cross sections. The Giessen crossed-beams experiment employs a high-power electron gun which has been developed over recent…

Atomic Physics · Physics 2026-03-11 B. Michel Döhring , Alexander Borovik , Kurt Huber , Alfred Müller , Stefan Schippers

It is argued that the next linear colliders can serve as W factories that may be exploited for precision tests on the properties of the massive gauge bosons. The connection between the probing of the symmetry breaking sector and precise…

High Energy Physics - Phenomenology · Physics 2016-09-06 F. Boudjema

After 10 years of steadily increasing the experimental precision at LEP/SLC, there is a strong demand on an update of existing programs for fermion pair production. We present a rederivation of the O(alpha) Bremsstrahlung corrections to…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Jack

In this paper we outline a proposal for a Linear Collider Facility as the next flagship project for CERN. It offers the opportunity for a timely, cost-effective and staged construction of a new collider that will be able to comprehensively…

High Energy Physics - Experiment · Physics 2025-06-23 H. Abramowicz , E. Adli , F. Alharthi , M. Almanza-Soto , M. M. Altakach , S. Ampudia Castelazo , D. Angal-Kalinin , J. A. Anguiano , R. B. Appleby , O. Apsimon , A. Arbey , O. Arquero , D. Attié , J. L. Avila-Jimenez , H. Baer , Y. Bai , 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. Besançon , D. Bett , T. Biekötter , S. Bilanishvili , B. Bilki , B. Bilki , J. Björklund 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 , 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 , B. Foster , N. Fourches , M. C. Fouz , C. D. Fu , K. Fujii , J. Fujimoto , B. Fuks , J. Fuster , N. Fuster-Martínez , M. Gabelmann , F. Gaede , M. Galletti , E. Gallo , S. Ganjour , M. V. Garzelli , C. G. R. Geddes , R. L. Geng , S. Gessner , I. D. Gialamas , B. Gimeno , J. Goldstein , M. Goncerz , A. J. Gonsalves , F. J. Gonzalez , D. González-Iglesias , J. Grames , P. Grannis , L. Gray , G. Grenier , H. Guler , H. E. Haber , K. Hamaguchi , N. Hamann , O. Hartbrich , N. M. Hartman , G. Hütsi , S. Heinemeyer , 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 , Y. Iiyama , A. Irles , A. Ishikawa , M. Ishino , I. P. Ivanov , M. Jacewicz , R. Jaramillo , D. Jeans , C. Jing , R. M Jones , W. Kaabi , M. Kagan , J. Kalinowski , D. K Kalvik , J. Kaminski , K. Kannike , A. Karam , Y. Kato , K. Kawagoe , D. Käfer , 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. Krüger , M. Kucharczyk , N. Kumar , Y. Kurihara , J. Kvasnicka , I. Laktineh , A. Latina , F. LeDiberder , A. Levy , M. Liepe , C. A. Lindstrøm , B. List , J. 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. Martín-Luna , A. Martens , V. J. Martin , L. Marzola , V. I. Maslov , K. T. Matchev , S. Matsumoto , K. Mawatari , J. P. Márquez , M. M. Mühlleitner , A. McIlvenny , P. A. McIntosh , K. Mekala , D. Melini , F. Meloni , A. Menéndez , K. Mimasu , V. Miralles , W. Mitaroff , V. A. Mitsou , L. Monaco , G. Moortgat-Pick , M. Moreno-Llácer , T. Mori , J. M. Moron , S. Morton , D. Moya , M. Mulder , 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. Núñez Pardo de Vera , M. Nojiri , D. Ntounis , A. Ody , O. M. Ogreid , T. Ohl , C. Oleari , M. Olvegård , 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. Pöschl , F. Peña , L. K Pedraza-Motavita , M. E. Peskin , F. Pilat , P. Piot , S. Plätzer , 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 , R. Ruber , S. Rudrabhatla , A. Ruiz Jimeno , Y. Sakaki , F. Salvatore , S. Sasikumar , T Schörner , A. Scheinker , S. Schroeder , C. B. 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 , K. Sugizaki , Z. Sun , T. Takahashi , T. Takeshita , T. Tauchi , G. Taylor , D. Terzani , T. Teubner , J. Tian , J. Timmermans , M. Titov , R. Tomas Garcia , T. Tong , J. M. Torndal , M. Trautwein , 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 , I. Vidakovic , H. Videau , I. Vila , M. Villaplana , M. Vos , N. Vukasinovic , N. Walker , K. Wandall-Christensen , Y. Wang , B. F. L. Ward , T. Watanabe , N. K. Watson , G. Weiglein , J. D. Wells , H. Wennlöf , M. Wenskat , S. Westhoff , J. W. Wetzel , A. P. White , P. H. Williams , M. Williams , G. W. Wilson , M. Wing , A. Winter , M. Winter , T. Wojton , J. C. Wood , W. Wuensch , X. Xia , H. Yamamoto , A. Yamamoto , K. Yamamoto , S. Yamashita , M. Yamauchi , M. Yoshioka , J. Zalesak , A. F. Zarnecki , K. Zembaczynski , D. Zerwas , W. Zhang , J. Zhang , Y. Zhang , M. Zielinski , M. Zobov

These proceedings outline steps toward a systematic analysis of frontier energy collider data: specifically, those data collected at Tevatron Runs I and II, LEP Run II, HERA Runs I and II, and the future LHC. Algorithms designed to…

High Energy Physics - Experiment · Physics 2009-11-10 Bruce Knuteson

We perform a detailed study of the process $e^+e^-\to \mu^+\mu^-\nu_l\bar\nu_l$ including all contributions. The contributions other than from real gauge boson production leads to a rich phenomenology. We explore the use of the process as a…

High Energy Physics - Phenomenology · Physics 2009-10-28 G. Couture , S. Godfrey

The prospects for electroweak precision measurements at the Future Circular Collider with electron-positron beams (FCC-ee) are discussed. The Z mass and width, as well as the value of the electroweak mixing angle, can be measured with very…

High Energy Physics - Experiment · Physics 2014-12-10 Roberto Tenchini

The measurement of Born cross section of $e^+e^-\to ZH$ process is one of the major goals of the future Circular Electron Positron Collider, which may reach a precision of 0.5%. Such unprecedented precision must be guaranteed by both…

High Energy Physics - Experiment · Physics 2019-07-24 Shuang Han , Gang Li , Xiang Zhou , Quan-Lin Jie

The total and differential cross sections of the process e+e- -> n gamma with n >= 2 are measured using data collected by the L3 experiment at centre-of-mass energies of \sqrt{s}=183 and 189 GeV. The results are in agreement with the…

High Energy Physics - Experiment · Physics 2012-08-27 L3 Collaboration

The precise knowledge of the QED initial state corrections is of instrumental importance in studying high luminosity measurements in $e^+e^-$ annihilation at facilities like LEP, the International Linear Collider ILC, CLIC, a Giga-$Z$…

High Energy Physics - Phenomenology · Physics 2022-05-11 J. Blümlein , K. Schönwald

The construction of two electron linacs and an optical FEL system is proposed. This facility, which would serve primarily as a Higgs-boson collider factory, could be built in two stages, each with distinct physics objectives requiring…

High Energy Physics - Experiment · Physics 2009-01-09 Radoje Belusevic

Lepto-nuclear colliders offer unique experimental opportunities to probe QCD in an extended medium. Of the many possibilities, three experiments are described here that are clearly feasible and of high scientific importance. First, a direct…

Nuclear Experiment · Physics 2010-11-19 W K Brooks

We discuss the need to compare total cross-section measurements at LHC and HERA with each other and with available models in order to obtain a more precise prediction of the total hadronic cross-section at the future Linear Collider, thus…

High Energy Physics - Phenomenology · Physics 2007-05-23 G. Pancheri , A. De Roeck , R. M. Godbole , A. Grau , Y. N. Srivastava

In this Report, QCD results obtained from a study of hadronic event structure in high energy e^+e^- interactions with the L3 detector are presented. The operation of the LEP collider at many different collision energies from 91 GeV to 209…

High Energy Physics - Experiment · Physics 2012-08-27 L3 Collaboration

At LEP~1, cross sections and cross section asymmetries may be analysed model independently. Cross sections depend on four, asymmetries on two free parameters. As an example, I discuss the model independent $Z$ boson mass determination from…

High Energy Physics - Phenomenology · Physics 2016-09-01 Tord Riemann

A promising avenue to perform precision tests of the SM at the LHC is to measure differential cross-sections at high invariant mass, exploiting in this way the growth with the energy of the corrections induced by heavy new physics. We…

High Energy Physics - Phenomenology · Physics 2018-06-11 Roberto Franceschini , Giuliano Panico , Alex Pomarol , Francesco Riva , Andrea Wulzer

We compute the total cross section as well as angular and energy distributions for process $e^+e^-\to\gamma\gamma\gamma$ with both unpolarized and polarized beams in the framework of noncommutative quantum electrodynamics (NCQED). The…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alberto Devoto , Stefano Di Chiara , Wayne W. Repko