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We study the Higgs self couplings of a supersymmetric $E_6$ model that has two Higgs doublets and two Higgs singlets. The lightest scalar Higgs boson in the model may be heavier than 112 GeV, at the one-loop level, where the negative…

High Energy Physics - Phenomenology · Physics 2009-12-01 S. W. Ham , Kideok Han , Jungil Lee , S. K. Oh

The ILD detector is proposed for an electron-positron collider with collision centre-of-mass energies from 90~\GeV~to about 1~\TeV. It has been developed over the last 10 years by an international team of scientists with the goal to design…

Instrumentation and Detectors · Physics 2020-03-04 The ILD Collaboration

Hadron colliders at the energy frontier offer significant discovery potential through precise measurements of Standard Model processes and direct searches for new particles and interactions. A future hadron collider would enhance the…

High Energy Physics - Experiment · Physics 2025-11-19 Viviana Cavaliere , Monica Dunford , Heather M. Gray , Elliot Lipeles , Alison Lister , Clara Nellist

Assuming that a Higgs sector is responsible for electroweak symmetry breaking, we attempt to address two important questions: How much better precision are various measurements of Higgs boson properties at a future linear collider than at…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Rainwater

Top quark production in the process $e^+e^- \rightarrow t\bar{t}$ at a future linear electron positron collider with polarised beams is a powerful tool to determine indirectly the scale of new physics. The presented study, based on a…

High Energy Physics - Experiment · Physics 2013-07-31 M. S. Amjad , M. Boronat , T. Frisson , I. Garcìa Garcìa , R. Pöschl , E. Ros , F. Richard , J. Rouëné , P. Ruiz Femenia , M. Vos

This work presents the status and plans of the International Large Detector (ILD) concept, one of the most detailed and comprehensive detector concepts for a future Higgs factory. Most hardware groups have demonstrated ILD's performance…

High Energy Physics - Experiment · Physics 2023-11-16 Ulrich Einhaus

In a class of Randall-Sundrum(RS) models, matter fermions and gauge bosons live in a five dimensional bulk, while the Higgs boson lives in a four dimensional visible brane. The Higgs boson can mix with a radion, by a Higgs-radion mixing…

High Energy Physics - Phenomenology · Physics 2016-11-02 Hirohisa Kubota , Mihoko Nojiri

Experiments at particle colliders have reached center of mass energies well above 100 GeV, equivalent to temperatures which existed shortly after the big bang. These experiments, testing the initial conditions of the universe have, with…

High Energy Physics - Experiment · Physics 2009-09-25 M. Dittmar

We first outline the Standard Model (SM) of particle physics, particle production and decay, and the expected signal and background at a Higgs factory like the International Linear Collider (ILC). We then introduce high energy colliders and…

High Energy Physics - Phenomenology · Physics 2020-05-12 C. T. Potter

The International Large Detector, ILD, is a detector concept which has been developed for the electron-positron collider ILC. The detector has been optimized for precision physics in a range of energies between 90 GeV and 1 TeV. ILD…

Instrumentation and Detectors · Physics 2019-12-11 The ILD Collaboration , contact Ties Behnke

Combined analyses at the Large Hadron Collider and at the International Linear Collider are important to reveal precisely the new physics model as, for instance, supersymmetry. Examples are presented where ILC results as input for LHC…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gudrid Moortgat-Pick

The successful operation of the Large Hadron Collider (LHC) and the excellent performance of the ATLAS, CMS, LHCb and ALICE detectors in Run-1 and Run-2 with $pp$ collisions at center-of-mass energies of 7, 8 and 13 TeV as well as the giant…

High Energy Physics - Phenomenology · Physics 2019-12-23 P. Azzi , S. Farry , P. Nason , A. Tricoli , D. Zeppenfeld , R. Abdul Khalek , J. Alimena , N. Andari , L. Aperio Bella , A. J. Armbruster , J. Baglio , S. Bailey , E. Bakos , A. Bakshi , C. Baldenegro , F. Balli , A. Barker , W. Barter , J. de Blas , F. Blekman , D. Bloch , A. Bodek , M. Boonekamp , E. Boos , J. D. Bossio Sola , L. Cadamuro , S. Camarda , F. Campanario , M. Campanelli , J. M. Campbell , Q. -H. Cao , V. Cavaliere , A. Cerri , G. S. Chahal , B. Chargeishvili , C. Charlot , S. -L. Chen , T. Chen , L. Cieri , M. Ciuchini , G. Corcella , S. Cotogno , R. Covarelli , J. M. Cruz-Martinez , M. Czakon , A. Dainese , N. P. Dang , L. Darmé , S. Dawson , H. De la Torre , M. Deile , F. Deliot , S. Demers , A. Denner , F. Derue , L. Di Ciaccio , W. K. Di Clemente , D. Dominguez Damiani , L. Dudko , A. Durglishvili , M. Dünser , J. Ebadi , R. B. Ferreira De Faria , G. Ferrera , A. Ferroglia , T. M. Figy , K. D. Finelli , M. C. N. Fiolhais , E. Franco , R. Frederix , B. Fuks , B. Galhardo , J. Gao , J. R. Gaunt , T. Gehrmann , A. Gehrmann-De Ridder , D. Giljanovic , F. Giuli , E. W. N. Glover , M. D. Goodsell , E. Gouveia , P. Govoni , C. Goy , M. Grazzini , A. Grohsjean , J. F. Grosse-Oetringhaus , P. Gunnellini , C. Gwenlan , L. A. Harland-Lang , P. F. Harrison , G. Heinrich , C. Helsens , M. Herndon , O. Hindrichs , V. Hirschi , A. Hoang , K. Hoepfner , J. M. Hogan , A. Huss , S. Jahn , Sa. Jain , S. P. Jones , A. W. Jung , H. Jung , S. Kallweit , D. Kar , A. Karlberg , T. Kasemets , M. Kerner , M. K. Khandoga , H. Khanpour , S. Khatibi , A. Khukhunaishvili , J. Kieseler , J. Kretzschmar , J. Kroll , E. Kryshen , V. S. Lang , L. Lechner , C. A. Lee , M. Leigh , D. Lelas , R. Les , I. M. Lewis , B. Li , Q. Li , Y. Li , J. Lidrych , Z. Ligeti , J. M. Lindert , Y. Liu , K. Lohwasser , K. Long , D. Lontkovskyi , G. Majumder , M. Mancini , P. Mandrik , M. L. Mangano , I. Marchesini , C. Mayer , K. Mazumdar , J. A. McFayden , P. M. Mendes Amaral Torres Lagarelhos , A. B. Meyer , S. Mikhalcov , S. Mishima , A. Mitov , M. Mohammadi Najafabadi , M. Moreno Llácer , M. Mulders , M. Myska , M. Narain , A. Nisati , T. Nitta , A. Onofre , S. Pagan Griso , D. Pagani , E. Palencia Cortezon , A. Papanastasiou , K. Pedro , M. Pellen , M. Perfilov , L. Perrozzi , B. A. Petersen , M. Pierini , J. Pires , M. -A. Pleier , S. Plätzer , K. Potamianos , S. Pozzorini , A. C. Price , M. Rauch , E. Re , L. Reina , J. Reuter , T. Robens , J. Rojo , C. Royon , S. Saito , A. Savin , S. Sawant , B. Schneider , R. Schoefbeck , M. Schoenherr , H. Schäfer-Siebert , M. Seidel , M. Selvaggi , T. Shears , L. Silvestrini , M. Sjodahl , K. Skovpen , N. Smith , D. Spitzbart , P. Starovoitov , C. J. E. Suster , P. Tan , R. Taus , D. Teague , K. Terashi , J. Terron , S. Uplap , F. Veloso , M. Verzetti , M. A. Vesterinen , V. E. Vladimirov , P. Volkov , G. Vorotnikov , M. Vranjes Milosavljevic , N. Vranjes , E. Vryonidou , D. Walker , M. Wiesemann , Y. Wu , T. Xu , S. Yacoob , E. Yazgan , J. Zahreddine , G. Zanderighi , M. Zaro , O. Zenaiev , G. Zevi Della Porta , C. Zhang , W. Zhang , H. L. Zhu , R. Zlebcik , F. N. Zubair

The Compact Linear Collider, CLIC, is a proposed e$^+$e$^-$ collider at the TeV scale whose physics potential ranges from high-precision measurements to extensive direct sensitivity to physics beyond the Standard Model. This document…

High Energy Physics - Experiment · Physics 2018-12-20 P. Roloff , R. Franceschini , U. Schnoor , A. Wulzer

This paper reviews the potential of a high luminosity e+e- linear collider (LC) in the precision study of the Higgs boson profile. The complementarity of the linear collider data with that from the LHC is also discussed together with a…

High Energy Physics - Phenomenology · Physics 2009-11-07 Marco Battaglia , Klaus Desch

A primary goal of present and future colliders is measuring the Higgs couplings to Standard Model (SM) particles. Any observed deviation from the SM predictions for these couplings is a sign of new physics whose energy scale can be bounded…

High Energy Physics - Phenomenology · Physics 2021-07-13 Fayez Abu-Ajamieh , Spencer Chang , Miranda Chen , Markus A. Luty

In this paper we study the effect of new physics contributions to the top quark pair production ($t\bar{t}$) in a possible future linear collider, such as the International Linear Collider (ILC). The use of a dimension-six gauge invariant…

High Energy Physics - Phenomenology · Physics 2013-03-22 Miguel C. N. Fiolhais

Due to the high energy and luminosity of the LHC, the ATLAS experiment has a huge discovery potential for new physics. A Standard Model Higgs boson can be discovered over the full range of allowed masses, and its mass should be measured…

High Energy Physics - Phenomenology · Physics 2017-08-23 V. A. Mitsou

The perspectives for measuring the top quark and the Higgs boson in nuclear collisions at the LHC and Future Circular Collider (FCC) are summarized. Perturbative QCD calculations at (N)NLO accuracy, including nuclear parton distribution…

High Energy Physics - Experiment · Physics 2017-01-30 David d'Enterria

The discovery of the Higgs boson at the LHC has opened the door to clarify the mechanism of electroweak symmetry breaking and the origin of masses of particles. The Higgs sector in the SM is the simplest but has no theoretical principle, so…

High Energy Physics - Phenomenology · Physics 2022-03-02 Shinya Kanemura

Measurement of the Higgs coupling to W-bosons is an important test of our understanding of the electroweak symmetry breaking mechanism. We study the sensitivity of the International Linear Collider (ILC) to the presence of anomalous HW+W-…

High Energy Physics - Phenomenology · Physics 2015-03-17 Yosuke Takubo , Robert N. Hodgkinson , Katsumasa Ikematsu , Keisuke Fujii , Nobuchika Okada , Hitoshi Yamamoto