Minimal spontaneously broken hidden sector and its impact on Higgs boson physics at the Large Hadron Collider
By A. Carrera, D. Evans, G. Zarnauskas, C. Eggel, Jose Manuel Zurita, P. Pereira, M. I. Jiménez, A. Castillo, S. Meola. 2008
180 citations recorded by the source corpus.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/11331973fed861c5e4f7ac45756849f470cf4c9a
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In Nuclear and High Energy Physics
- Atlas Collaboration
- Cms Collaboration
- Gudrun Heinrich
- Stefan Dittmaier
- Ansgar Denner
- M. Grazzini
- Fabio Maltoni
- M. Schönherr
Citations in the corpus
- Higgs boson self-coupling measurements using ratios of cross sections (2013, background): “As we have already discussed at the end of Section 2, such situations may arise in Higgs Portal or TwoHiggs Doublets Models.”
- Building and testing models with extended Higgs sectors (2017, background): “This simple and far-reaching idea of the Higgs plus gauge singlet scalar combination as a portal to a new hidden world was explicitly articulated in [347], although models exploiting such interaction appeared earlier [109, 110, 348].”
- Handbook of LHC Higgs Cross Sections: 3. Higgs Properties (2013, background): “2 The model The most general gauge-invariant potential can be written a s [617,619]”
- Searching for long-lived particles beyond the Standard Model at the Large Hadron Collider (2019, background): “This naturally yields high-multiplicity events featuring particles with a hierarchy of lifetimes [32, 230, 456].”
- Illuminating dark photons with high-energy colliders (2014, background): “The importance of an additional Higgs portal coupling to sectors containing a dark vector boson has been realized before [68, 91], particularly in the context of hidden valley models [92].”
- Higgs singlet extension parameter space in the light of the LHC discovery (2013, methodology): “The decay width Γ and coupling strength μ′ of the H → hh decay are [8, 29]: Γ (H → hh) = |μ ′|2 8πmH √ 1− 4m(2)h m(2)H , μ′ = −3 2 ( x cos(3) α+ v sin(3) α ) + (λ3 − 3λ1) v cos(2) α sin α + (λ3 − 3λ2) x cos α sin(2) α.”
- Beyond the Standard Model Physics at the HL-LHC and HE-LHC (2018, methodology): “Examples of such models include hidden valley models [346,728], the NMSSM [528] or Higgs portal scenarios [729].”