We report a transition from a homogeneous steady state (HSS) to inhomogeneous
steady states (IHSSs) in a network of globally coupled identical oscillators.
We perturb a synchronized population in the network with a few local negative
mean field links. It is observed that the whole population splits into two
clusters for a certain number of negative mean field links and specific range
of coupling strength. For further increases of the strength of interaction
these clusters collapse to a HSS followed by a transition to IHSSs. We
analytically determine the origin of HSS and its transition to IHSS in relation
to the number of negative mean-field links and the strength of interaction
using a reductionism approach to the model network in a two-cluster state. We
verify the results with numerical examples of networks using the paradigmatic
Landau-Stuart limit cycle system and the chaotic Rossler oscillator as
dynamical nodes. During the transition from HSS to IHSSs, the network follows
the Turing type symmetry breaking pitchfork or transcritical bifurcation
depending upon the system dynamics.Comment: 6 pages, 5 figures, accepted in Chaos: An Interdisciplinary Journal
of Nonlinear Scienc