Vectorlike confinement at the LHC
By C. Kilic, Takemichi Okui, R. Sundrum. 2009
135 citations recorded by the source corpus.
We argue for the plausibility of a broad class of vectorlike confining gauge theories at the TeV scale which interact with the Standard Model predominantly via gauge interactions. These theories have a rich phenomenology at the LHC if confinement occurs at the TeV scale, while ensuring negligible impact on precision electroweak and flavor observables. Spin-1 bound states can be resonantly produced via their mixing with Standard Model gauge bosons. The resonances promptly decay to pseudo-Goldstone bosons, some of which promptly decay to a pair of Standard Model gauge bosons, while others are charged and stable on collider time scales. The diverse set of final states with little background include multiple photons and leptons, missing energy, massive stable charged particles and the possibility of highly displaced vertices in dilepton, leptoquark or diquark decays. Among others, a novel experimental signature of resonance reconstruction out of massive stable charged particles is highlighted. Some of the long-lived states also constitute Dark Matter candidates.
Subfields: Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/13b89c60e9bf1958c3847f87968a9c7613a4912a
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In Nuclear and High Energy Physics
Citations in the corpus
- Accidental composite dark matter (2015, background): “Usually such singlets undergo decays into pairs of SM gauge bosons through chiral anomalies [4]; when present their axion-like couplings to photons provides a mild constraint on their mass (that need to be larger than a keV) and a production mechanism at colliders.”
- A composite model for the 750 GeV diphoton excess (2015, background): “assignment was also considered in [6].”
- Dynamical generation of the weak and Dark Matter scales from strong interactions (2014, background): “The LHC phenomenology of techni-strong dynamics was discussed in [1].”
- What is the γγ resonance at 750 GeV? (2015, background): “We now consider QCD-like strongly coupled sectors that do not break the electroweak symmetry [46].”