  From lattice-regularized models, devoid of any non-Hermitian (NH) skin
effects, here we compute the electrical ($\sigma_{xy}$), thermal
($\kappa_{xy}$), and spin ($\sigma^{sp}_{xy}$) Hall, and the electrical
($G_{xx}$) and thermal ($G^{th}_{xx}$) longitudinal conductivities for
appropriate NH planar topological insulators and superconductors related to all
five non-trivial Altland-Zirbauer symmetry classes in the Hermitian limits.
These models feature real eigenvalues over an extended NH parameter regime,
only where the associated topological invariants remain quantized. In this
regime, the NH quantum anomalous and spin Hall insulators show quantized
$\sigma_{xy}$ and $G_{xx}$, respectively, the NH $p+ip$ ($p \pm ip$) pairing
shows half-quantized $\kappa_{xy}$ ($G^{th}_{xx}$), while the NH $d+id$ pairing
shows quantized $\kappa_{xy}$ and $\sigma^{sp}_{xy}$ in the clean and weak
disorder (due to random pointlike charge impurities) regimes. We compute these
quantities in experimentally realizable suitable six-terminal setups using the
Kwant software package. But, in the strong disorder regime, all these
topological responses vanish and with the increasing non-Hermiticity in the
system this generic phenomenon occurs at weaker disorder.
