  We investigate a Randall-Sundrum model with an SU(2) doublet propagating in
the bulk. Upon calculating its gravitational effect we find that a stabilized
radius can be generated without the use of an additional scalar, as needed for
example in the Goldberger-Wise (GW) mechanism, and with no additional
fine-tuning other than the inescapable one due to the cosmological constant;
similar tuning is also present in the GW mechanism. The lowest scalar
excitation in this scenario, the counterpart of the radion of the GW mechanism,
has both radion-like and Higgs-like couplings to the SM fields. It, thus, plays
a dual role and we, therefore, denote it as the "Higgs-radion" ($h_r$). As
opposed to the GW radion case, our Higgs-radion is found to be compatible with
the 126 GeV scalar recently discovered at the LHC, at the level of $1\sigma$,
with a resulting $95\%$ CL bound on the KK-gluon mass of: $4.48~TeV<M_{KKG}<
5.44~TeV$. An important consequence of our setup should be accentuated: the
radion of the traditional RS scenarios simply does not exist, so that our
Higgs-radion is not the conventional mixed state between the GW radion and the
Higgs.
