On the phenomenology of a two-Higgs-doublet model with maximal CP symmetry at the LHC. Part II: radiative effects

Maniatis M, Nachtmann O (2010)
Journal of High Energy Physics 2010(4).

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The processes p (p) over bar and pp -> gamma + heavy-flavour jet(s) + X are studied in the framework of a special two-Higgs-doublet model, the MCPM. As distinguishing feature of this model we find that radiative Higgs-boson production and decay lead to heavy flavour c jets but no b jets in the above processes. Thus, the prediction is that b jets should be given by the normal QCD processes whereas for c jets an excess over the QCD expectation should occur. We present results both for Tevatron and LHC energies.
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Maniatis M, Nachtmann O. On the phenomenology of a two-Higgs-doublet model with maximal CP symmetry at the LHC. Part II: radiative effects. Journal of High Energy Physics. 2010;2010(4).
Maniatis, M., & Nachtmann, O. (2010). On the phenomenology of a two-Higgs-doublet model with maximal CP symmetry at the LHC. Part II: radiative effects. Journal of High Energy Physics, 2010(4).
Maniatis, M., and Nachtmann, O. (2010). On the phenomenology of a two-Higgs-doublet model with maximal CP symmetry at the LHC. Part II: radiative effects. Journal of High Energy Physics 2010.
Maniatis, M., & Nachtmann, O., 2010. On the phenomenology of a two-Higgs-doublet model with maximal CP symmetry at the LHC. Part II: radiative effects. Journal of High Energy Physics, 2010(4).
M. Maniatis and O. Nachtmann, “On the phenomenology of a two-Higgs-doublet model with maximal CP symmetry at the LHC. Part II: radiative effects”, Journal of High Energy Physics, vol. 2010, 2010.
Maniatis, M., Nachtmann, O.: On the phenomenology of a two-Higgs-doublet model with maximal CP symmetry at the LHC. Part II: radiative effects. Journal of High Energy Physics. 2010, (2010).
Maniatis, Markos, and Nachtmann, O. “On the phenomenology of a two-Higgs-doublet model with maximal CP symmetry at the LHC. Part II: radiative effects”. Journal of High Energy Physics 2010.4 (2010).
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