2015/06/30 by Sebastian Ohmer, Hiren H. Patel · 1 citation
Physics and Astronomy · #Black Holes and Theoretical Physics #Dark matter #Fermion #Higgs boson #MAJORANA #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #hep-ph
paper · pdf · doi:10.1103/physrevd.92.055020
published as Phys. Rev. D 92, 055020 (2015) · 15 pages, 10 figures; v3: corrected typos, to appear in PRD
arxiv created 2015/09/04 · openalex publication_date 2015/09/16 · arxiv updated 2015/09/23 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We explore the dark matter and collider phenomenology of the minimal gauged U(1)B model, consisting of a leptophobic ZB gauge boson, and an accompanying Higgs SB. By requirement of anomaly cancellation, the fermion sector naturally contains a dark matter candidate---a Majorana isosinglet \ensuremathχ stabilized by an inherent Z2 symmetry. The absence of evidence for Z prime dijet resonances at the LHC suggests that the scale of symmetry breaking is \mathrm\ensuremathΛB\ensuremath\gtrsim500 GeV. Saturation of dark matter abundance together with limits on the direct detection cross section (dominated by Higgs exchange) constrains the Higgs mixing angle to |\ensuremathθ|\ensuremath\lesssim0.22. For small mixing angles of |\ensuremathθ|\ensuremath\lesssim10^\ensuremath-3, the O(10%) branching fractions of the fermion loop-mediated SB\ensuremath→\ensuremathγ\ensuremathγ, Z\ensuremathγ, ZZ modes may provide clues about the fermion content of the model at the LHC.