Towards testing a two-Higgs-doublet model with maximal CP symmetry at the LHC: Monte Carlo event generator implementation
A Monte Carlo event generator is implemented for a two-Higgs-doublet model with maximal CP symmetry, the MCPM. The model contains five physical Higgs bosons; the ρ′, behaving similarly to the standard-model Higgs boson, two extra neutral bosons h′ and h″, and a charged pair H±. The special feature o...
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| Hauptverfasser: | , , , , , |
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| Dokumenttyp: | Article (Journal) |
| Sprache: | Englisch |
| Veröffentlicht: |
3 April 2013
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| In: |
The European physical journal. C, Particles and fields
Year: 2013, Jahrgang: 73 |
| ISSN: | 1434-6052 |
| DOI: | 10.1140/epjc/s10052-013-2380-3 |
| Online-Zugang: | Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1140/epjc/s10052-013-2380-3
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| Verfasserangaben: | J. Brehmer, V. Lendermann, M. Maniatis, O. Nachtmann, H.-C. Schultz-Coulon, R. Stamen |
MARC
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| 245 | 1 | 0 | |a Towards testing a two-Higgs-doublet model with maximal CP symmetry at the LHC |b Monte Carlo event generator implementation |c J. Brehmer, V. Lendermann, M. Maniatis, O. Nachtmann, H.-C. Schultz-Coulon, R. Stamen |
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| 520 | |a A Monte Carlo event generator is implemented for a two-Higgs-doublet model with maximal CP symmetry, the MCPM. The model contains five physical Higgs bosons; the ρ′, behaving similarly to the standard-model Higgs boson, two extra neutral bosons h′ and h″, and a charged pair H±. The special feature of the MCPM is that, concerning the Yukawa couplings, the bosons h′, h″ and H± couple directly only to the second-generation fermions but with strengths given by the third-generation-fermion masses. Our event generator allows the simulation of the Drell-Yan-type production processes of h′, h″ and H± in proton-proton collisions at LHC energies. Also the subsequent leptonic decays of these bosons into the μ+μ−, μ+νμand $\mu^{-} \bar{\nu}_{\mu}$channels are studied as well as the dominant background processes. We estimate the integrated luminosities needed in pp collisions at center-of-mass energies of 8 and 14 TeV for significant observations of the Higgs bosons h′, h″ and H± in these muonic channels. | ||
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