  We study the fractionally quantized $Z_N$ Berry phase, $\gamma_N=0, {2\pi
\over N}, {4\pi \over N},\ldots, {2(N-1)\pi \over N}$, to characterize local
$N$-mer spin structures at magnetization plateaux in spin-1/2 Heisenberg
multimer ($N$-mer) models, i.e., highly frustrated $N$-leg ladder models, which
are generalizations of an orthogonal dimer chain and have exact ground states
in the strong multimer coupling region. We demonstrate that all $N$ types of
Berry phases, which characterize magnetization-plateau phases, appear in a
magnetic phase diagram when $N=2$ and $4$. We show that magnetization plateau
with magnetization $\langle m\rangle$ and $D$-fold degenerated states has
$\gamma_N=\pi (\langle m\rangle-1) D$, except for the Haldane phase with
$\gamma_N=0$. In addition, we find that a complementary $Z_N$ Berry phase
becomes non-zero in the $S=N/2$ Haldane phase for $N=2$ and 4. Because the
exact quantization of the $Z_N$ Berry phases is protected by the translational
(or rotational) symmetry along the rung direction, the $Z_N$ Berry phase has
the potential to be applied for a wide class of magnetization plateaux in
coupled multimer systems.
