We report on the discovery of a transition in rings of coupled electro
nic circuits in the chaotic regime to a collective periodic state char
acterized by a time scale that is between two and three orders faster
than that corresponding to an isolated circuit. This transition arises
from a linear instability in the uniform synchronized state of the ri
ng through a symmetric Hopf bifurcation. The same type of transition i
s also observed for other coupled chaotic systems, e.g., a ring of Lor
enz attractors.