
Weakly Connected Oscillatory Networks
■
447
with s
ij
=C
ij
V (ω)B
j
. It is readily derived that phase configurations such that
(
j
−
i
) ∈{0, π} are equilibrium points of (17.33), i.e., in-phase or anti-phase–
locked states are admissible steady-state solutions. This agrees with the assumption
that function (17.32) satisfies condition (17.31).
By remembering that each limit cycle (either stable or unstable) of the WCON
corresponds to an equilibrium point of the phase equation, the coefficients s
ij
can
be designed according to a simple learning rule in order to store a given set of phase
patterns.
14
The parameters C
ij
of the coupling function (17.32), which defines ...