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Flavonstrahlung in the $B_3-L_2$ $Z'$ Model at Current and Future Colliders
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abstract
The $B_3-L_2$ $Z^\prime$ model may explain some gross features of the fermion mass spectrum as well as $b\rightarrow s \ell \ell$ anomalies. A TeV-scale physical scalar field associated with gauged $U(1)_{B_3-L_2}$ spontaneous symmetry breaking, the flavon field $\vartheta$, affects Higgs phenomenology via mixing. In this paper, we investigate the collider phenomenology of the flavon field. Higgs and $W$ boson mass data are used to place bounds upon parameter space. We then examine flavonstrahlung (${Z^\prime} \rightarrow Z^\prime \vartheta$ production) at colliders as a means to directly produce and discover flavon particles, providing direct empirical evidence tying it to $U(1)_{B_3-L_2}$ symmetry breaking. A 100 TeV FCC-hh or a 10 TeV muon collider would have high sensitivity to flavonstrahlung, whereas the HL-LHC can observe it only in extreme corners of parameter space.
Forward citations
Cited by 2 Pith papers
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Constraints on the malaphoric $B_3-L_2$ model from di-lepton resonance searches at the LHC
New bounds from ATLAS 13 TeV di-lepton searches force the malaphoric B3-L2 Z' to exceed 2.8 TeV to preserve its b to s l+ l- fit, and the HL-LHC is expected to reach 4.2 TeV.
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The Plan B Model: $Z^{\prime}$ collider phenomenology and discovery prospects
Current LHC data exclude a significant portion of the Plan B Model's preferred parameter space, and the HL-LHC could extend sensitivity to Z′ masses around 2.5 TeV.
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