  Plasma response to resonant magnetic perturbations (RMPs) near the pedestal
top is crucial for accessing edge localized modes (ELMs) suppression in
tokamaks. Since radial location of rotation zero-crossing plays a key role in
determining the threshold for field penetration of RMP, plasma response may be
different in low input torque plasmas. In this work, the linear MHD code MARS-F
is applied to reveal the dependence of plasma response to RMP on rotation
zero-crossing by a scan of rotation profiles based on an EAST equilibrium. It
is shown that the plasma response is enhanced when zero-crossing occurs near
rational surfaces. The dependence of plasma response on the location of
rotation zero-crossing is well fitted by a double Gaussian, indicating two
effects in this enhancement. One is induced by rotation screening effect shown
as a wide base (with a width around 10-20 krad/s), and the other is related to
resistive singular layer effect characterized by a localized peak (with a width
around 3-4 krad/s). The width of the peak scales with the resistive singular
layer width. The plasma displacement suggests the response is tearing like when
zero-crossing is within the singular layer, while it is kink like when
zero-crossing is far from the layer. The enhancement of magnetic islands width
at the peak is only around a factor of two, when the absolute value of local
rotation is not larger than 10-20 krad/s. It is further confirmed in a modeling
of plasma response in an EAST ELM suppression discharge. Though there is a
zero-crossing in $E\times B$ rotation but not in electron perpendicular
rotation, no significant difference in plasma response is obtained using these
two rotation profiles. This suggests that the rotation near pedestal top should
not be far away from zero but may not be necessary to have zero-crossing for
accessing ELM suppression.
