  We further elaborate on the proposal that the Higgs boson should be a broad
heavy resonance, referred to as true Higgs $H_T$, with mass around $750 \,
GeV$.
  We stress once again that within the Standard Model the true Higgs is the
unique possibility to implement the spontaneous symmetry breaking of the local
gauge symmetry by elementary, relativistic and strictly local scalar fields. We
discuss the most relevant decay modes of the $H_T$ boson and estimate they
partial decay widths and branching ratios. We discuss briefly the experimental
signatures of the $H_T$ Higgs boson and compare with the recent available LHC
data at $\sqrt{s} =13 \,TeV$. We find that the coupling of the $H_T$ Higgs
boson to fermions is strongly suppressed.
  We also compare our theoretical expectations in the so-called golden channel
to the data collected by the ATLAS and CMS Collaborations at $\sqrt{s} =13
\,TeV$ with an integrated luminosity of $36.1 \, fb^{-1}$ and $35.9 \, fb^{-1}$
respectively. We find that our theoretical expectations are in fair good
agreement with the experimental observations. Combining the data from both the
LHC Collaborations we obtain an evidence of the heavy Higgs boson in this
channel with an estimated statistical significance of more than three standard
deviations. Finally, we argue that, if the signal is real, by the end of the
Run 2 both the LHC experiments will reach in the golden channel a statistical
significance of about five standard deviations.
