We analyze the parity-time (
P
T
) symmetric phase in coupled two waveguides with a Kerr-type medium in between. Paying attention to the emitted field from a dipole source inside, we show that when the strength of the dipole increases, the optical Kerr effect can render a phase transition from the exact
P
T
phase to the broken
P
T
phase. Furthermore, a salient phenomenon of bistable-like
P
T
phase is observed, in which the emitted field possesses a paradox between the two kinds of
P
T
phases. We show that the physical mechanism of this bistable-like phenomenon is a globally inhomogeneous
P
T
phase, in which different spatial regions of the whole structure can possess different
P
T
phases (broken or exact). This study highlights the potential to manipulate the
P
T
phase transition by using optical nonlinearity for many interesting applications.