Generating the Electro-Weak Scale by Vector-like Quark Condensation
arXiv:2205.15323 · doi:10.21468/SciPostPhys.14.4.076
Abstract
We show that vector-like quarks in the fundamental or higher-dimensional representations of QCD can generate the electro-weak scale in a phenomenologically viable way by chiral symmetry breaking condensates. The thereby generated scales are determined by numerically solving the Dyson-Schwinger equation and these scales are sizable, because they grow with the hard vector-like mass. Communicating such a scale to the Standard Model via a conformally invariant scalar sector can dynamically generate the electro-weak scale without a naturalness problem, because all non-dynamical mass scales are protected by chiral symmetry. We present a minimal setup which requires only a new neutral scalar with mass not too far above the electro-weak scale, as well as vector-like quarks at the (multi-)TeV scale. Both are consistent with current bounds and are attractive for future experimental searches at the LHC and future colliders. Depending on the hypercharge of the vector-like quarks, hadrons made of them are color-neutral bound states which would be interesting Dark Matter candidates.
19 pages, 9 figures, 1 table
References in corpus (11)
- The QCD Equation of State with almost Physical Quark Masses
- Conformal Symmetry and the Standard Model
- Electroweak Symmetry Breaking induced by Dark Matter
- Scale invariant extension of the standard model with strongly interacting hidden sector
- Electroweak Higgs as a pseudo-Goldstone boson of broken scale invariance
- Propagators and phase structure of Nf=2 and Nf=2+1 QCD
- Search for heavy charged long-lived particles in the ATLAS detector in 36.1 fb of proton-proton collision data at TeV
- Direct determination of the strange and light quark condensates from full lattice QCD
- QCD phase transitions via a refined truncation of Dyson-Schwinger equations
- New insight on the quark condensate beyond chiral limit
- Extracting the condensate for light quarks beyond the chiral limit in models of QCD