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In many extensions of the standard model, there exist a few extra Higgs bosons. Suppose a heavy neutral Higgs boson H is discovered at the LHC, one could then investigate CP and CPT~ properties of its couplings to a pair of $Z$ bosons…

High Energy Physics - Phenomenology · Physics 2018-01-17 Jung Chang , Kingman Cheung , Jae Sik Lee , Chih-Ting Lu , Jubin Park

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

One of the central goals of the physics program at the future colliders is to elucidate the origin of electroweak symmetry breaking, including precision measurements of the Higgs sector. This includes a detailed study of Higgs boson (H)…

The measurement of the triple Higgs coupling is a key benchmark for the LHC and future colliders. It directly probes the Higgs potential and its fundamental properties in connection to new physics beyond the Standard Model. There exist two…

High Energy Physics - Phenomenology · Physics 2018-10-25 Dorival Goncalves , Tao Han , Felix Kling , Tilman Plehn , Michihisa Takeuchi

The conjoined production at the LHC of single top and Higgs boson via $t$-channel weak boson exchange is ideal to probe the top-quark Yukawa coupling, due to a delicate cancellation between the amplitudes with the $htt$ and the $hWW$…

High Energy Physics - Phenomenology · Physics 2019-02-27 Vernon Barger , Kaoru Hagiwara , Ya-Juan Zheng

The final state obtained when a Higgs boson decays to a photon and a Z boson has been mostly overlooked in current searches for a light Higgs boson. However, when the Z boson decays leptonically, all final state particles in this channel…

High Energy Physics - Phenomenology · Physics 2015-03-19 James S. Gainer , Wai-Yee Keung , Ian Low , Pedro Schwaller

We discuss some aspects of the interplay between the top quark and the Higgs boson at the LHC. First we describe what indirect information on the top Yukawa coupling can be extracted from measurements in the Higgs sector. We then show that…

High Energy Physics - Phenomenology · Physics 2015-06-15 Mikael Chala , Jose Santiago

Machine learning techniques are used for treating jets as images to explore the performance of boosted top quark tagging. Tagging performances are studied in both hadronic and leptonic channels of top quark decay, employing a convolutional…

High Energy Physics - Phenomenology · Physics 2022-02-22 Soham Bhattacharya , Monoranjan Guchait , Aravind H. Vijay

The $CP$ properties of the coupling between the Higgs boson and the top quark are investigated with 139 fb$^{-1}$ of proton-proton collision data recorded by the ATLAS experiment at the LHC at a centre-of-mass energy of $\sqrt{s}=13$ TeV.…

High Energy Physics - Experiment · Physics 2024-04-17 ATLAS Collaboration

We consider top-antitop quark $(t{\bar t})$ production at the Large Hadron Collider (LHC) with subsequent decays into dileptonic final states. We use and investigate a set of leptonic angular correlations and distributions with which all…

High Energy Physics - Phenomenology · Physics 2024-05-30 Werner Bernreuther , Long Chen , Zong-Guo Si

Extra Higgs states appear in various scenarios beyond the current Standard Model of elementary particles. If discovered at the LHC or future colliders, the question will arise whether CP is violated or conserved in the extended scalar…

High Energy Physics - Phenomenology · Physics 2021-04-07 Stefan Antusch , Oliver Fischer , A. Hammad , Christiane Scherb

The discovery of the Higgs boson in 2012, by the ATLAS and CMS experiments, was a success achieved with only a percent of the entire dataset foreseen for the LHC. It opened a landscape of possibilities in the study of Higgs boson…

High Energy Physics - Phenomenology · Physics 2019-03-20 M. Cepeda , S. Gori , P. Ilten , M. Kado , F. Riva , R. Abdul Khalek , A. Aboubrahim , J. Alimena , S. Alioli , A. Alves , C. Asawatangtrakuldee , A. Azatov , P. Azzi , S. Bailey , S. Banerjee , E. L. Barberio , D. Barducci , G. Barone , M. Bauer , C. Bautista , P. Bechtle , K. Becker , A. Benaglia , M. Bengala , N. Berger , C. Bertella , A. Bethani , A. Betti , A. Biekotter , F. Bishara , D. Bloch , P. Bokan , O. Bondu , M. Bonvini , L. Borgonovi , M. Borsato , S. Boselli , S. Braibant-Giacomelli , G. Buchalla , L. Cadamuro , C. Caillol , A. Calandri , A. Calderon Tazon , J. M. Campbell , F. Caola , M. Capozi , M. Carena , C. M. Carloni Calame , A. Carmona , E. Carquin , A. Carvalho Antunes De Oliveira , A. Castaneda Hernandez , O. Cata , A. Celis , A. Cerri , F. Cerutti , G. S. Chahal , A. Chakraborty , G. Chaudhary , X. Chen , A. S. Chisholm , R. Contino , A. J. Costa , R. Covarelli , N. Craig , D. Curtin , L. D'Eramo , N. P. Dang , P. Das , S. Dawson , O. A. De Aguiar Francisco , J. de Blas , S. De Curtis , N. De Filippis , H. De la Torre , L. de Lima , A. De Wit , C. Delaere , M. Delcourt , M. Delmastro , S. Demers , N. Dev , R. Di Nardo , S. Di Vita , S. Dildick , L. A. F. do Prado , M. Donadelli , D. Du , G. Durieux , M. Dührssen , O. Eberhardt , K. El Morabit , J. Elias-Miro , J. Ellis , C. Englert , R. Essig , S. Falke , M. Farina , A. Ferrari , A. Ferroglia , M. C. N. Fiolhais , M. Flechl , S. Folgueras , E. Fontanesi , P. Francavilla , R. Franceschini , R. Frederix , S. Frixione , G. Gómez-Ceballos , A. Gabrielli , S. Gadatsch , M. Gallinaro , A. Gandrakota , J. Gao , F. M. Garay Walls , T. Gehrmann , Y. Gershtein , T. Ghosh , A. Gilbert , R. Glein , E. W. N. Glover , R. Gomez-Ambrosio , R. Gonçalo , D. Gonçalves , M. Gorbahn , E. Gouveia , M. Gouzevitch , P. Govoni , M. Grazzini , B. Greenberg , K. Grimm , A. V. Gritsan , A. Grohsjean , C. Grojean , J. Gu , R. Gugel , R. S. Gupta , C. B. Gwilliam , S. Höche , M. Haacke , Y. Haddad , U. Haisch , G. N. Hamity , T. Han , L. A. Harland-Lang , R. Harnik , S. Heinemeyer , G. Heinrich , B. Henning , V. Hirschi , K. Hoepfner , J. M. Hogan , S. Homiller , Y. Huang , A. Huss , S. Jézéquel , Sa. Jain , S. P. Jones , K. Köneke , J. Kalinowski , J. F. Kamenik , M. Kaplan , A. Karlberg , M. Kaur , P. Keicher , M. Kerner , A. Khanov , J. Kieseler , J. H. Kim , M. Kim , T. Klijnsma , F. Kling , M. Klute , J. R. Komaragiri , K. Kong , J. Kozaczuk , P Kozow , C. Krause , S. Lai , J. Langford , B. Le , L. Lechner , W. A. Leight , K. J. C. Leney , T. Lenz , C-Q. Li , H. Li , Q. Li , S. Liebler , J. Lindert , D. Liu , J. Liu , Y. Liu , Z. Liu , D. Lombardo , A. Long , K. Long , I. Low , G. Luisoni , L. L. Ma , A. -M. Magnan , D. Majumder , A. Malinauskas , F. Maltoni , M. L. Mangano , G. Marchiori , A. C. Marini , A. Martin , S. Marzani , A. Massironi , K. T. Matchev , R. D. Matheus , K. Mazumdar , J. Mazzitelli , A. E. Mcdougall , P. Meade , P. Meridiani , A. B. Meyer , E. Michielin , P. Milenovic , V. Milosevic , K. Mimasu , B. Mistlberger , M. Mlynarikova , M. Mondragon , P. F. Monni , G. Montagna , F. Monti , M. Moreno Llacer , A. Mueck , P. C. Muiño , C. Murphy , W. J. Murray , P. Musella , M. Narain , R. F. Naranjo Garcia , P. Nath , M. Neubert , O. Nicrosini , K. Nikolopoulos , A. Nisati , J. M. No , M. L. Ojeda , S. A. Olivares Pino , A. Onofre , G. Ortona , S. Pagan Griso , D. Pagani , E. Palencia Cortezon , C. Palmer , C. Pandini , G. Panico , L. Panwar , D. Pappadopulo , M. Park , R. Patel , F. Paucar-Velasquez , K. Pedro , L. Pernie , L. Perrozzi , B. A. Petersen , E. Petit , G. Petrucciani , G. Piacquadio , F. Piccinini , M. Pieri , T. Plehn , S. Pokorski , A. Pomarol , E. Ponton , S. Pozzorini , S. Prestel , K. Prokofiev , M. Ramsey-Musolf , E. Re , N. P. Readioff , D. Redigolo , L. Reina , E. Reynolds , M. Riembau , F. Rikkert , T. Robens , R. Roentsch , J. Rojo , N. Rompotis , J. Rorie , J. Rosiek , J. Roskes , J. T. Ruderman , N. Sahoo , S. Saito , R. Salerno , P. H. Sales De Bruin , A. Salvucci , K. Sandeep , J. Santiago , R. Santo , V. Sanz , U. Sarica , A. Savin , A. Savoy-Navarro , S. Sawant , A. C. Schaffer , M. Schlaffer , A. Schmidt , B. Schneider , R. Schoefbeck , M. Schröder , M. Scodeggio , E. Scott , L. Scyboz , M. Selvaggi , L. Sestini , H. -S. Shao , A. Shivaji , L. Silvestrini , L. Simon , K. Sinha , Y. Soreq , M. Spannowsky , M. Spira , D. Spitzbart , E. Stamou , J. Stark , T. Stefaniak , B. Stieger , G. Strong , M. Szleper , K. Tackmann , M. Takeuchi , S. Taroni , M. Testa , A. Thamm , V. Theeuwes , L. A. Thomsen , S. Tkaczyk , R. Torre , F. Tramontano , K. A. Ulmer , T. Vantalon , L. Vecchi , R. Vega-Morales , E. Venturini , M. Verducci , C. Vernieri , T. Vickey , M. Vidal Marono , P. Vischia , E. Vryonidou , P. Wagner , V. M. Walbrecht , L. -T. Wang , N. Wardle , D. R. Wardrope , G. Weiglein , S. Wertz , M. Wielers , J. M. Williams , R. Wolf , A. Wulzer , M. Xiao , H. T. Yang , E. Yazgan , Z. Yin , T. You , F. Yu , G. Zanderighi , D. Zanzi , M. Zaro , S. C. Zenz , D. Zerwas , M. Zgubič , J. Zhang , L. Zhang , W. Zhang , X. Zhao , Y. -M. Zhong

In the presence of CP violation, the Higgs-top coupling may have both scalar and pseudoscalar components, $\kappa_t$ and ${\tilde \kappa_t}$, which are bounded indirectly but only weakly by the present experimental constraints on the…

High Energy Physics - Phenomenology · Physics 2015-06-18 John Ellis , Dae Sung Hwang , Kazuki Sakurai , Michihisa Takeuchi

We evaluate the discovery potential for the heavy Higgs bosons at the LHC energy upgrade with $\sqrt{s}=27$ TeV. We take degenerate mass spectrum and assume near the alignment limit in the Type-II Two Higgs Doublet Model for illustration.…

High Energy Physics - Phenomenology · Physics 2019-05-27 Tong Li

The H to tau tau decays form the prime channel for the measurement of the Higgs boson state and tests of the CP invariance of Higgs boson couplings. A previous study has shown the viability of deep learning techniques for the measurement.…

High Energy Physics - Phenomenology · Physics 2017-10-11 Elisabetta Barberio , Brian Le , Elzbieta Richter-Was , Zbigniew Was , Daniele Zanzi , Jakub Zaremba

We study the LHC sensitivity to new broad neutral resonances produced in two-photon fusion and decaying to a top quark pair, $\gamma\gamma \to t\bar{t}$. This is probed in central exclusive $t\bar{t}$ production in proton-proton collisions,…

High Energy Physics - Phenomenology · Physics 2022-08-24 Cristian Baldenegro , Andrea Bellora , Sylvain Fichet , Gero von Gersdorff , Michael Pitt , Christophe Royon

Search for the Higgs Boson is one of the prime goals of the LHC. Higgs bosons lighter than 130 GeV decay mainly to a b-quark pair. While the detection of a directly produced Higgs boson in the bb channel is impossible because of the huge…

High Energy Physics - Phenomenology · Physics 2007-05-23 V. Drollinger , T. Muller , D. Denegri

Top polarization is an important probe of new physics that couples to the top sector, and which may be discovered at the 14 TeV LHC. Taking the example of the MSSM, we argue that top polarization measurements can put a constraint on the…

High Energy Physics - Phenomenology · Physics 2013-03-28 Biplob Bhattacherjee , Sourav K. Mandal , Mihoko Nojiri

With a high instantaneous luminosity and the large top quark pair production cross section, the Large Hadron Collider (LHC) will be a "top factory" allowing the analysis of millions of top events. After a short description of the top quark…

High Energy Physics - Experiment · Physics 2007-05-23 Florian Beaudette

Precision measurements of top-associated Higgs production are an important ingredient to unravel the $\mathcal{CP}$ nature of the Higgs boson. In this work, we constraint the $\mathcal{CP}$ nature of the top-Yukawa coupling taking into…

High Energy Physics - Phenomenology · Physics 2021-07-23 Henning Bahl
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