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Related papers: HERWIG for Top Physics at the Linear Collider

200 papers

The current status of top quark studies at the Large Hadron Collider (LHC) and at the Linear Collider (LC) is summarized. Expectations on the measurements of the top mass, couplings and decays, of the top spin polarization and of the single…

High Energy Physics - Experiment · Physics 2009-12-10 Marina Cobal

I discuss charged-Higgs production via two different processes: in association with a top quark, and in association with a $W$ boson. I present total cross sections and differential distributions that include higher-order corrections from…

High Energy Physics - Phenomenology · Physics 2018-08-10 Nikolaos Kidonakis

Some aspects of the phenomenology of the top quark and the charged Higgs are studied, emphasizing relations due to radiative corrections. Production mechanisms at the SSC are mentioned, and decay modes are analyzed including radiative…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marco A. Diaz

The process $e^+e^-\to H t\bar t$ can be used at the Next Linear Collider to measure the Higgs-top Yukawa coupling. In this paper, we compute $2\to 8$ processes of the form $e^+e^-\to b\bar b b\bar b W^+W^-\to b\bar b b\bar b…

High Energy Physics - Phenomenology · Physics 2009-10-31 Stefano Moretti

In this study, Higgs production processes, Higgsstrahlung and vector boson (W and Z) fusion processes, were investigated for four different future lepton colliders (CEPC, ILC, CLIC, and FCC-ee). The cross sections for each production…

High Energy Physics - Phenomenology · Physics 2023-02-01 Deniz Yilmaz , Mehmet Sahin , Dogukan Hazar Yavuz

At small x, the gluon distribution dominates the nuclear wave function. The increase needs to be tamed in avoid violating unitarity constraints. The most efficient way to study this in colliders is through e+A collisions as the nucleus is…

Nuclear Experiment · Physics 2008-07-02 Matthew Lamont

I review standard top quark production at the Fermilab Tevatron. The current theoretical understanding of the total cross section and many partial differential cross sections is presented. Studies on the effects of extra gluon radiation on…

High Energy Physics - Phenomenology · Physics 2009-10-28 Stephen Parke

The theoretical predictions in the MSSM for Higgs-boson production at a future e^+e^- Linear Collider and Higgs-boson decay processes are discussed focusing in particular on recent diagrammatic two-loop results in the MSSM Higgs sector. The…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. Heinemeyer , G. Weiglein

I present higher-order radiative corrections from collinear and soft gluon emission for the associated production of a charged Higgs boson with a $W$ boson. The calculation uses expressions from resummation at next-to-leading-logarithm…

High Energy Physics - Phenomenology · Physics 2018-02-07 Nikolaos Kidonakis

For an electron-photon collider the complete tree-level cross sections of the reaction $\gamma e \rightarrow \nu b \bar{b} W$ are computed at center-of-mass energies between 0.5 and 2.0 TeV, for top masses of 160 to 200 GeV and Higgs masses…

High Energy Physics - Phenomenology · Physics 2011-07-19 E. Boos , A. Pukhov , M. Sachwitz , H. J. Schreiber

The physics potential is briefly summarized for an e+e- linear collider operating at center-of-mass energies up to \sqrt{s} = 1 TeV and delivering integrated luminosities up to \int L = 0.5 ab^(-1) in one to two years. This machine will…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. M. Zerwas

Electroweak processes in high-energy lepton collisions are considered in a situation where the incident center-of-mass energy lies below the reaction threshold, but is boosted to the required level by subsequent laser acceleration. Within…

High Energy Physics - Phenomenology · Physics 2014-02-27 Sarah J. Müller , Christoph H. Keitel , Carsten Müller

We review exclusive top pair production including decays at a future high-energy lepton collider, both in the threshold region and for higher energies. For the continuum process, we take complete QCD next-to-leading order matrix elements…

We discuss vector boson production at hadron colliders and the treatment of the initial-state radiation according to Monte Carlo parton shower simulations and resummed calculations. In particular, we investigate the effect of matrix-element…

High Energy Physics - Phenomenology · Physics 2009-10-31 Gennaro Corcella

The ECFA Higgs, electroweak, and top Factory Study ran between 2021 and 2025 as a broad effort across the experimental and theoretical particle physics communities, bringing together participants from many different proposed future collider…

High Energy Physics - Experiment · Physics 2025-10-20 H. Abidi , J. A. Aguilar-Saavedra , S. Airen , S. Ajmal , M. Al-Thakeel , G. L. Alberghi , J. Alcaraz Maestre , J. Alimena , S. Alshamaily , J. Altmann , W. Altmannshofer , Y. Amhis , A. Amiri , A. Andreazza , S. Antusch , O. Arnaez , K. A. Assamagan , S. Aumiller , K. Azizi , P. Azzi , P. Azzurri , E. Bagnaschi , Z. Baharyioon , H. Bahl , V. Balagura , D. Barducci , M. J. Basso , P. Bechtle , L. Bellagamba , M. Berggren , G. Bernardi , J. Bhom , L. Biermann , F. Blekman , B. Bliewert , M. Bordone , V. Boudry , D. Boye , I. Bozovic , J. Braathen , J. -C. Brient , G. Brodbek , E. Brost , P. Bruckman , B. Brudnowski , M. Bulliri , E. Bulyak , J. M. Burridge , P. N. Burrows , D. Buttazzo , G. Cacciapaglia , V. Cairo , O. Cakir , A. C. Canbay , F. Canelli , J. M. Carceller , C. Carloni Calame , N. F. Castro , V. Cavaliere , E. Celada , F. G. Celiberto , M. Cepeda , G. Chachamis , M. Chala , C. Charlot , H. -C. Cheng , M. Chiesa , M. Chrzaszcz , W. Chung , M. Cobal , I. Combes , A. E. Connelly , C. Cornella , F. Cornet-Gomez , I. Corredoira , A. J. Costa , T. Critchley , E. Curtis , D. d'Enterria , M. Dam , V. Dao , A. Das , S. Dasu , J. Davighi , J. de Blas , N. De Filippis , A. De Moor , A. De Vita , M. M. Defranchis , C. L. Del Pio , M. Delmastro , H. Denizli , A. Desai , K. Dewyspelaere , M. Di Carlo , S. D. Dittmaier , D. Dobur , A. Dondarini , M. Drewes , B. Dudar , H. Duran Yildiz , G. Durieux , J Dutta , U. Einhaus , W. Elmetenawee , C. Englert , F. Erben , B. A. Erdelyi , J. Eysermans , S. Farrington , H. Fatehi , A. Filipe Silva , M. C. Fouz , R. Franceschini , B. Francois , A. Freitas , K. Fujii , J. Fuster , M. G. Gabelmann , F. Gaede , A. Gallén , G. Ganis , D. Garcia , S. Gascon-Shotkin , K. Gautam , Y. Georis , S. Giappichini , P. Goldenzweig , R. Gonzalez Suarez , E. G. Gorini , L. Gouskos , F. G. Grancagnolo , L. Gray , R. Gröber , A. Greljo , A. V. Gritsan , A. Grohsjean , C. Grojean , J. Gu , G. Guerrieri , J. Hajer , C. Hays , J. Hayward , S. Heinemeyer , K. Hidaka , G. Iakovidis , A. Ilg , A. Irles , M. Ishino , G. Isidori , A. Jafari , R. Jafariseyedabad , A. Jüttner , D. Jeans , X. -H. Jiang , E. Jourd'huy , G. Kacarevic , A. Kaczmarska , J. Kalinowski , K. Köneke , S. Keilbach , M. Kenzie , V. Keus , H. Khanpour , J. Kieseler , W. Kilian , B. Kilminster , J. Klamka , J. Klarić , M. Klute , P. Kontaxakis , P. Koppenburg , A. Korajac , K. Kröninger , S. Kuberski , M. Kucharczyk , T. H. Kwok , T. Lagouri , J Lahiri , M. Larson , C. Leonidopoulos , T. Lesiak , A. Li , C. Li , L. Li , J. Liao , J. List , P. Lo Chiatto , V. Lukashenko , A. Lusiani , Y. Ma , A. Macchiolo , R. Madar , T. Madlener , A. -M. Magnan , P. Malecki , M. Malekhosseini , A. Maloizel , F. Maltoni , L. S. Mandacarú Guerra , L. Mantani , G. Marchiori , G. Marino , D. Marzocca , J. P. Márquez , A. Mehta , K. Mekala , C. Meroni , F. Mescia , A. B. Meyer , G. Milutinovic-Dumbelovic , K. M. Mimasu , V. Miralles , T. Miralles , M. Miralles López , W. Mitaroff , V. A. Mitsou , A. Mohammadi , M. Mohammadi Najafabadi , G. Montagna , S. Monteil , G. Moortgat-Pick , N. Morange , M. Moreno Llácer , T. Mori , K. Mota Amarilo , T. Murata , E. Musumeci , J. Nakajima , S. Narita , M. T. Núñez Pardo de Vera , C. -H Nee , J. Nesbitt , A. Nesterenko , O. Nicrosini , M. Nourbakhsh , D. Ntounis , C. Ochando , T. Ohl , N. Okada , V. A. Okorokov , B. M. S. Oliveira , W. Ootani , M. Ouchemhou , F. Palla , P. Panci , O. Panella , G. Panizzo , B. Pattnaik , R. Pöschl , R. Perez-Ramos , F. Piccinini , A. Pilkington , M. Pinamonti , N. Pinto , L. Pintucci , S. Plaetzer , V. Plakkot , M. A. Pleier , E. Ploerer , G. Polesello , Z. Polonsky , P. Poulose , M. Presilla , A. Price , M. P. Primavera , F. M. Procacci , D. Protopopescu , W. Płaczek , K. Radchenko Serdula , L. Röhrig , M. Reboud , L. Reichenbach , S. Renner , J. Reuter , F. Richard , G. Ripellino , T. Robens , A. Robson , J. Rojo , A. Rossia , S. Rostami , M. Ruan , A. Ruiz Jimeno , F. Sabatini , A. Sabio Vera , A. Saibel , A. Sailer , K. Sakurai , R. Salerno , M. A. Sanchis , S. Sasikumar , D. Schulte , A. Schwartzman , R. Schwienhorst , A. Sciandra , F. Sefkow , T. Seino , N. Selimović , M. Selvaggi , A. Senol , A. Sfyrla , Y. Shi , A. Siódmok , J. Silva , F. Simon , Y. Sirois , T. Sjöstrand , P. Skands , L. Skinnari , K. Skovpen , M. Skrzypek , V. Slokenbergs , J. Smiesko , I. Smiljanic , S. Snyder , Y. Soreq , M. Spira , T. Suehara , O. Sumensari , R. H. Szafron , M. Szewc , R. Tagami , H. Taibi , T. Takeshita , M. Tammaro , M. D. Tat , J. ter Hoeve , M. Thomas , S. Thor , J. Tian , A. Tishelman-Charny , S. Tizchang , L. Toffolin , A. Tolosa-Delgado , J. Torndal , J. T. Tsang , I. Turk Cakir , M. Tytgat , F. Ucci , N. Valle , M. Vande Voorde , I. Velišček , M. Vellasco , A. Verduras Schaeidt , C. Vernieri , C. Verollet , A. Vicini , I. Vidakovic , M. Vos , E. Vryonidou , N. Vukasinovic , B. F. L. Ward , N. Wardle , Z. Was , G. Weiglein , X. -K. Wen , A. R. Wiederhold , A. Wiedl , G. Wilkinson , S. Williams , G. W. Wilson , Z. Wu , J. Xiao , B. Yan , F. Yu , Z. Yu , C. -P. Yuan , R. Zanzottera , A. F. Zarnecki , M. Zaro , K. Zembaczynski , D. Zerwas , Y. Zhang , Y. Zhang , X. Zuo , J. Zurita

The HERWIG event generator was widely used throughout the workshop, particularly in the emulation of Supersymmetric and Higgs processes in the context of the Minimal Supersymmetric Standard Model. We briefly review here its main features in…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Moretti

A future linear collider will complement the programme of the Large Hadron Collider, especially for precision physics. The RADCOR community has an important part to play in refining the predictions for rates and processes in Electroweak,…

High Energy Physics - Experiment · Physics 2007-05-23 D. J. Miller

The talk summarises the case for Higgs physics in $e^+e^-$ collisions and explains how Higgs parameters can be extracted in a model-independent way at the International Linear Collider (ILC). The expected precision will be discussed in the…

High Energy Physics - Experiment · Physics 2014-10-14 Felix Sefkow

We study standard electroweak/Higgs processes at the high-energy lepton colliders ILC and CLIC. We identify a subset of three operators in the SMEFT that give leading contributions to these processes at high energies. We then perform a…

High Energy Physics - Phenomenology · Physics 2022-02-24 Shankha Banerjee , Rick S. Gupta , Oscar Ochoa-Valeriano , Michael Spannowsky

Superconducting technology makes it possible to build a high energy $e^+e^-$ linear collider with energy recovery (ERLC) and reusable beams. To avoid parasitic collisions inside the linacs, a twin (dual) LC is proposed. In this article, I…

Accelerator Physics · Physics 2023-06-21 V. I. Telnov