“…Physical Properties. The physical properties of K Z P~( C N )~X~.~( H Z O )~-(X = C1, Br) have been extensively analyzed in terms of several models for highly conducting one-dimensional systems undergoing a metal-insulator transition including interrupted strands (120,173,253,344,345,346,434) and disorder dominated transport (50,51,336,472). These materials are currently best understood in terms of the physical model of a band conductor undergoing a Peierls transition (433) to a semiconductor as the temperture is lowered (433) with evidence for the presence of a pinned charge density wave (Frohlich collective mode) below 200°K (457).…”