When a discrete nonlinear array is driven across a periodic surface spatial
ly coherent modes of motion can coexist associated with different average v
elocities due to resonant parametric forcing of the particle fluctuations b
y the center of mass motion. Depending on the coupling strength kappa and s
ize of the array N, jumps in the minimum friction (maximum velocity) exhibi
ted by the array occur at kappa(m)(N) similar to (N/m)(2) as new modes stab
ilize and are selected by the dynamics. The existence of such coherent mode
s allows both an effective low dimensional description of the dynamics to e
xist and the possibility for control of friction close to these instabiliti
es.