  The high frequency limits of the singular component $A(\omega)$ of the small
wavevector expansion of the longitudinal (L) and transverse (T) components of
the spin-resolved exchange-correlation kernel tensor $f_{xc,\sigma
\sigma'}^{L,T}(q,\omega)=-v(q)G_{\sigma \sigma'}^{L,T}(q,\omega)$ in a
two-dimensional isotropic electron liquid with arbitrary spin polarization are
studied. Here $G_{\sigma \sigma'}^{L,T}(q,\omega)$ is the spin-resolved local
field factor, $v(q)$ is the Coulomb interaction in momentum space, and $\sigma$
denotes spin. Particularly, the real part of $A(\omega)$ is found to be
logarithmically divergent at large $\omega$. the large wavevetor structure of
the corresponding spin-resolved static structure factor is also established.
