2012/04/30 by A. Djouadi, Abdelhak Djouadi, Alexander Lenz · 129 citations
Physics and Astronomy · #Boson #Cosmology and Gravitation Theories #Dark Matter and Cosmic Phenomena #Electroweak interaction #Fermion #Higgs boson #Large Hadron Collider #Nuclear physics #Particle physics #Particle physics theoretical and experimental studies #Physics #Tevatron #hep-ex #hep-ph
paper · pdf · doi:10.1016/j.physletb.2012.07.060
published in Physics Letters B 715(4-5), 310-314 (Elsevier BV) · 8 pages, 3 figures; Discussion of the recent Higgs results in a Note added
arxiv created 2012/07/04 · openalex publication_date 2012/08/01 · arxiv updated 2015/06/04 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/08
The search for the effects of heavy fermions in the extension of the Standard Model with a fourth generation is part of the experimental program of the Tevatron and LHC experiments. Besides being directly produced, these states affect drastically the production and decay properties of the Higgs boson. In this note, we first reemphasize the known fact that in the case of a light and long-lived fourth neutrino, the present collider searches do not permit to exclude a Higgs boson with a mass below the WW threshold. In a second step, we show that the recent results from the ATLAS and CMS collaborations which observe an excess in the γγ and 4ℓ^± search channels corresponding to a Higgs boson with a mass MH ≈ 125 GeV, cannot rule out the fourth generation possibility if the H → γγ decay rate is evaluated when naively implementing the leading \cal O(GF mf'2) electroweak corrections. Including the exact next-to-leading order electroweak corrections leads to a strong suppression of the H → γγ rate and makes this channel unobservable with present data. Finally, we point out that the observation by the Tevatron collaborations of a \gsim 2σ excess in the mass range MH = 115-135 GeV in the channel q q → WH → Wb b can definitely not be accommodated by the fourth generation fermion scenario. All in all, if the excesses observed at the LHC and the Tevatron are indeed due to a Higgs boson, they unambiguously exclude the perturbative fermionic fourth generation case. In passing, we also point out that the Tevatron excess definitely rules out the fermiophobic Higgs scenario as well as scenarios in which the Higgs couplings to gauge bosons and bottom quarks are significantly reduced.