  The experimental and theoretical implications of heavy digauge boson
resonances that couple to, or are comprised of, new charged and strongly
interacting matter are investigated. Observation and measurement of ratios of
the resonant digauge boson channels $WW$, $ZZ$, $\gamma \gamma$, $Z \gamma$,
and $gg$ in the form of dijets, provide a rather direct -- and for some ratios
a rather robust -- probe of the gauge representations of the new matter. For a
spin-zero resonance with the quantum numbers of the vacuum, the ratios of
resonant $WW$ and $ZZ$ to $\gamma \gamma$ channels, as well as the longitudinal
versus transverse polarization fractions in the $WW$ and $ZZ$ channels, provide
probes for possible mixing with the Higgs boson, while di-Higgs and ditop
resonant channels, $hh$ and $tt$, provide somewhat less sensitivity. We present
a survey of possible underlying models for digauge boson resonances by
considering various limits for the mass of the new charged and strongly
interacting matter fields as well as the confinement scale of new hypergauge
interactions under which they may also be charged. In these limits, resonances
may be included as elementary weakly coupled spin-zero states or can correspond
to hyperglueballs, hyperonia, or pseudoscalar hypermesons. For each of these
cases, we make predictions for additional states that could be resonantly or
pair produced and observed at the Large Hadron Collider or in future collider
experiments. Heavy digauge boson resonances can provide a unified explanation
for a number of small discrepancies and excesses in reported data from the
Large Hadron Collider.
