scale and $\tilde g$ is a large coupling. Interactions of the resonances with other gauge bosons and fermions are calculated as a series in $1/\tilde g \ll 1$.

-   Standard model (SM) fermions reside primarily on the exterior sites – the sites approximately corresponding to $SU(2)_w$ and $U(1)_Y$ gauge groups. Fermions become massive through mixing with massive, vector-like fermions located on the interior, ‘hidden’ sites.

-   Precision electroweak parameters (S,T,U), perennially a thorn in the side of dynamical electroweak breaking models [@Peskin:1991sw], are accommodated by delicately spreading the SM fermions between sites. By adjusting the fermion distribution across sites to match the gauge boson distribution, S, T, U can all be reduced to acceptable levels. This is identical to the solution used in extra-dimensional Higgsless models, where the spreading of a fermion among sites becomes a continuous distribution, or profile, in the extra dimension [@Cacciapaglia:2006gp]. This adjustment is called “ideal delocalization” [@Chivukula:2005xm].

The most economical deconstructed Higgsless model constructed along these lines (a “three site” model) was presented in [@Chivukula:2006cg], and had, in addition to the SM spectrum, one heavy partner for each fermion and the $W$ and $Z$ bosons. Though providing an excellent ground for studying the low-energy properties 