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Related papers: Indirect sensitivity to Z's in high-energy e+e- co…

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We explore new physics (NP) effects in Higgs-Vector boson associated production at a future International Linear Collider (ILC) via e+e- -> Zh,Zhh, using effective field theory (EFT) techniques. In particular, we focus on a certain class of…

High Energy Physics - Phenomenology · Physics 2016-10-07 Jonathan Cohen , Shaouly Bar-Shalom , Gad Eilam

Based on Ref.[1], we study a composite Z' model which effectively induces the Stueckelberg model in low energy. It turns out that the mass of the composite Z' boson contains the Stueckelberg mass term in sharp contrast to the conventional…

High Energy Physics - Phenomenology · Physics 2015-05-01 Michio Hashimoto

Appreciable CP Asymmetries (~ 10%) can arise in the reaction e+ e- -> t bar-t Z already at TREE-LEVEL in models with two Higgs doublets. For a neutral Higgs particle, h, with a mass in the range 50 GeV < m_h < 400 GeV, it may be possible to…

High Energy Physics - Phenomenology · Physics 2009-10-30 S. Bar-Shalom , D. Atwood , A. Soni

Recent reports from the Large Hadron Collider indicate two excesses: one in the lighter Higgs mass region around 95 GeV, and another in the rare $Z \gamma$ final state of the Standard Model (SM) 125 GeV Higgs decay. These anomalies are…

High Energy Physics - Phenomenology · Physics 2025-07-03 Abdesslam Arhrib , Khiem Hong Phan , Van Que Tran , Tzu-Chiang Yuan

There are many possibilities for new physics beyond the Standard Model that feature non-standard Higgs sectors. These may introduce new sources of CP violation, and there may be mixing between multiple Higgs bosons or other new scalar…

High Energy Physics - Phenomenology · Physics 2022-10-26 S. Kraml , E. Accomando , A. G. Akeroyd , E. Akhmetzyanova , J. Albert , A. Alves , N. Amapane , M. Aoki , G. Azuelos , S. Baffioni , A. Ballestrero , V. Barger , A. Bartl , P. Bechtle , G. Belanger , A. Belhouari , R. Bellan , A. Belyaev , P. Benes , K. Benslama , W. Bernreuther , M. Besancon , G. Bevilacqua , M. Beyer , M. Bluj , S. Bolognesi , M. Boonekamp , F. Borzumati , F. Boudjema , A. Brandenburg , T. Brauner , C. P. Buszello , J. M. Butterworth , M. Carena , D. Cavalli , G. Cerminara , S. Y. Choi , B. Clerbaux , C. Collard , J. A. Conley , A. Deandrea , S. De Curtis , R. Dermisek , A. De Roeck , G. Dewhirst , M. A. Diaz , J. L. Diaz-Cruz , D. D. Dietrich , M. Dolgopolov , D. Dominici , M. Dubinin , O. Eboli , J. Ellis , N. Evans , L. Fano , J. Ferland , S. Ferrag , S. P. Fitzgerald , H. Fraas , F. Franke , S. Gennai , I. F. Ginzburg , R. M. Godbole , T. Gregoire , G. Grenier , C. Grojean , S. B. Gudnason , J. F. Gunion , H. E. Haber , T. Hahn , T. Han , V. Hankele , C. Hays , S. Heinemeyer , S. Hesselbach , J. L. Hewett , K. Hidaka , M. Hirsch , W. Hollik , D. Hooper , J. Hosek , J. Hubisz , C. Hugonie , J. Kalinowski , S. Kanemura , V. Kashkan , T. Kernreiter , W. Khater , V. A. Khoze , W. Kilian , S. F. King , O. Kittel , G. Klamke , J. L. Kneur , C. Kouvaris , M. Krawczyk , P. Krstonosic , A. Kyriakis , P. Langacker , M. P. Le , H. -S. Lee , J. S. Lee , M. C. Lemaire , Y. Liao , B. Lillie , V. Litvin , H. E. Logan , B. McElrath , T. Mahmoud , E. Maina , C. Mariotti , P. Marquard , A. D. Martin , K. Mazumdar , D. J. Miller , P. Mine , K. Moenig , G. Moortgat-Pick , S. Moretti , M. M. Muhlleitner , S. Munir , R. Nevzorov , H. Newman , P. Niezurawski , A. Nikitenko , R. Noriega-Papaqui , Y. Okada , P. Osland , A. Pilaftsis , W. Porod , H. Przysiezniak , A. Pukhov , D. Rainwater , A. Raspereza , J. Reuter , S. Riemann , S. Rindani , T. G. Rizzo , E. Ros , A. Rosado , D. Rousseau , D. P. Roy , M. G. Ryskin , H. Rzehak , F. Sannino , E. Schmidt , H. Schroder , M. Schumacher , A. Semenov , E. Senaha , G. Shaughnessy , R. K. Singh , J. Terning , L. Vacavant , M. Velasco , A. Villanova del Moral , F. von der Pahlen , G. Weiglein , J. Williams , K. Williams , A. F. Zarnecki , D. Zeppenfeld , D. Zerwas , P. M. Zerwas , A. R. Zerwekh , J. Ziethe

The models of large extra compact dimensions, as suggested by Arkani-Hamed, Dimopoulos and Dvali, predict exciting phenomenological consequences with gravitational interactions becoming strong at the TeV scale. Such theories can be tested…

High Energy Physics - Phenomenology · Physics 2009-11-10 N. G. Deshpande , Dilip Kumar Ghosh

The presence of extra scalar singlets is a feature of several motivated extensions of the Standard Model, and the mixing of such a singlet with the Higgs boson is allowed to be quite large by current experiments. In this paper we perform a…

High Energy Physics - Phenomenology · Physics 2016-01-20 Dario Buttazzo , Filippo Sala , Andrea Tesi

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

I review the physics of the Higgs sector in the Standard Model and its minimal supersymmetric extension, the MSSM. I will discuss the prospects for discovering the Higgs particles at the upgraded Tevatron, at the Large Hadron Collider, and…

High Energy Physics - Phenomenology · Physics 2016-09-06 Abdelhak Djouadi

The Z-pole data from e+e- colliders and results from the NuTeV experiment at Fermilab can be brought into agreement if (1) the neutrino-Z couplings were suppressed relative to the Standard Model (SM), and (2) the Higgs boson were much…

High Energy Physics - Phenomenology · Physics 2017-08-23 Tatsu Takeuchi , Will Loinaz , Naotoshi Okamura , L. C. R. Wijewardhana

We examine the sensitivity of $e \gamma$ colliders (based on $e^+ e^-$ linear colliders of c.m. energy 500 GeV) to the anomalous couplings of the Higgs to W-bosons via the process $e^- \gamma \longrightarrow \nu W H$. This has the advantage…

High Energy Physics - Phenomenology · Physics 2008-11-26 Debajyoti Choudhury , Mamta

Effective Field Theories (EFTs) capture effects from heavy dynamics at low energy and represent an essential ingredient in the context of Standard Model (SM) precision tests. This document gathers a number of relevant scenarios for heavy…

High Energy Physics - Phenomenology · Physics 2020-09-04 D. Marzocca , F. Riva , J. Criado , S. Dawson , J. de Blas , B. Henning , D. Liu , C. Murphy , M. Perez-Victoria , J. Santiago , L. Vecchi , Lian-Tao Wang

We consider the capability of a future high energy $e^+ e^-$ collider to search for the $Z^\prime$ bosons associated with a $U(1)^\prime$ gauge extension of the Standard Model. Even for $Z^\prime$ masses well above the center of mass energy…

High Energy Physics - Phenomenology · Physics 2015-06-18 David Kapukchyan , Tim M. P. Tait

New heavy neutral gauge bosons Z' are predicted by many models of physics beyond the Standard Model. It is quite possible that Z's are heavy enough to lie beyond the discovery reach of the CERN Large Hadron Collider LHC, in which case only…

High Energy Physics - Phenomenology · Physics 2015-06-05 V. V. Andreev , G. Moortgat-Pick , P. Osland , A. A. Pankov , N. Paver

We give a brief review of recent developments in non-supersymmetric models for electroweak symmetry breaking, including little Higgs, composite Higgs and Higgsless theories. The new ideas such as extra dimensions, AdS/CFT correspondence,…

High Energy Physics - Phenomenology · Physics 2007-10-19 Hsin-Chia Cheng

We describe the physics potential of $e^+e^-$ linear colliders in this report. These machines are planned to operate in the first phase at a center-of --mass energy of 500 GeV, before being scaled up to about 1 TeV. In the second phase of…

High Energy Physics - Phenomenology · Physics 2009-09-25 E. Accomando

Measuring the Higgs couplings accurately at colliders is one of the best routes for finding physics Beyond the Standard Model (BSM). If the measured couplings deviate from the SM predictions, then this would give rise to energy-growing…

High Energy Physics - Phenomenology · Physics 2022-07-06 Fayez Abu-Ajamieh

We argue that in the minimal supersymmetric extension of the Standard Model with a large trilinear coupling both the fundamental Higgs boson and a bound state of squarks (formed via strong scalar interaction) can have a non-zero VEV. This…

High Energy Physics - Phenomenology · Physics 2009-10-31 Gian F. Giudice , Alexander Kusenko

The impact of theoretical and experimental uncertainties on the indirect determination of the Higgs boson mass, MH, in the Standard Model (SM) is discussed. Special emphasis is put on the electroweak precision observables MW (the W boson…

High Energy Physics - Phenomenology · Physics 2007-05-23 U. Baur , R. Clare , J. Erler , S. Heinemeyer , D. Wackeroth , G. Weiglein , D. R. Wood

Motivated by the coupling unification problem, we propose a novel extension of the Minimal Supersymmetric Standard Model. One of the predictions of this extension is existence of new states neutral under SU(3)_c X SU(2)_w but charged under…

High Energy Physics - Theory · Physics 2009-10-31 Zurab Kakushadze