  This paper extends an earlier one describing the Higgs boson $H$ as a light
composite scalar in a strong extended technicolor model of electroweak symmetry
breaking. The Higgs mass $M_H$ is made much smaller than $\Lambda_{ETC}$ by
tuning the ETC coupling very close to the critical value for electroweak
symmetry breaking. The technicolor interaction, neglected in the earlier paper,
is considered here. Its weakness relative to extended technicolor is essential
to understanding the lightness of $H$ compared to the low-lying spin-one
technihadrons. Technicolor cannot be completely ignored, but implementing
technigluon exchange together with strong extended technicolor appears
difficult. We propose a solution that turns out to leave the results of the
earlier paper essentially unchanged. An argument is then presented that masses
of the spin-one technifermion bound states, $\rho_H$ and $a_H$, are much larger
than $M_H$ and, plausibly, controlled by technicolor. Assuming $M_{\rho_H}$ and
$M_{a_H}$ are in the TeV-energy region, we identify $\rho_H$ and $a_H$ with the
diboson excesses observed near $2\,{\rm TeV}$ by ATLAS and CMS in LHC Run 1
data, and we discuss their phenomenology for Runs 2 and 3.
