Aspects of the dynamics of walking technicolor models are expected to have important conszquences for technihadron production at hadron colliders. Hard-mass enhancements characteristic of walking technicolor raise technipion (n,) masses relative to technirho (p,) masses so that the decays pr--t'?T~'?T~ are either suppressed or forbidden altogether. Thus, p r can be unusually narrow with unconventional decay modes. Large weak isospin breaking in U-and D-technifermion masses (required for t-b splitting) leads to neutral p, and '?T, that are ideally mixed. Finally, multiscale models of walking technicolor in which the light-scale technifermions carry ordinary SU(3) color can have color-octet p,'s which are produced strongly in parton-parton collisions and are within reach of the Fermilab Tevatron. These would appear as narrow, well-separated pDD and pa, resonances in dijet production or in TTPT production with a limited number of final states. These expectations are illustrated in a multiscale model containing both techniquarks and technileptons at the light scale. Depending on assumptions that determine the fundamental chiral-symmetry-breaking mass parameters of the model, we find two generic phenomenologies: (A) p~~ with a mass of 20C250 GeV decaying exclusively to dijets and p,, in the mass range 350-550 GeV decaying to a few TTTT combinations; (B) pDD with a mass of 375425 GeV and p~, in the mass range 500-700 GeV both decaying to a few r~r~ modes. The p~, --tdijet signal of case A is large at all colliders and can be sought now at the Tevatron. The '~T,'?TT production rates in both cases are of -10 pb at the Tevatron and -10 nb at the Superconducting Super Collider (SSC). The technipions can be sought in the next high-luminosity run of the Tevatron and may be excludable if backgrounds are not too severe. Experiments at the SSC certainly should be able to determine whether they exist.

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