Flavonstrahlung in the B <inf>3</inf> − L <inf>2</inf> Z′ model at current and future colliders

Abstract

Abstract The B3− L2Z′ model may explain some gross features of the fermion mass spectrum as well as b → sℓℓ anomalies. A TeV-scale physical scalar field associated with gauged $$ U{(1)}_{B_3-{L}_2} $$ U 1

B 3

−

L 2

spontaneous symmetry breaking, the flavon field ϑ, 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′ → Z′ϑ production) at colliders as a means to directly produce and discover flavon particles, which would provide direct empirical evidence tying the flavon to $$ U{(1)}_{B_3-{L}_2} $$ 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.