  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 relevant 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 plasma. 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
$10-20~\mathrm{krad/s}$), and the other is related to resistive singular layer
effect characterized by a localized peak (with a width around
$3-4~\mathrm{krad/s}$). The peak of each resonant harmonic in plasma response
appears always at rotation zero-crossing. 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 the characteristic width around
$10-20~\mathrm{krad/s}$. 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.
