Displacement current is present where the electric field is time-dependent. In Region I, the electric field is given by \(E_x = E_0 \sin(kz - \omega t)\). The term \(-\omega t\) indicates this field's time variation. The displacement current density \(J_d\) is defined as \(J_d = \epsilon_0 \frac{\partial E_x}{\partial t}\).
Differentiating \(E_x\) with respect to time yields \(\frac{\partial E_x}{\partial t} = -\omega E_0 \cos(kz - \omega t)\).
Consequently, a displacement current exists in Region I. In Regions II, III, and IV, the electric field is static, meaning no displacement current is present.
Therefore, displacement current is found in:
\[\boxed{\text{Region I}}.\]