  To understand the relation between the chiral symmetry breaking and
monopoles, the chiral condensate which is the order parameter of the chiral
symmetry breaking is calculated in the $\overline{\mbox{MS}}$ scheme at 2
[GeV]. First, we add one pair of monopoles, varying the monopole charges
$m_{c}$ from zero to four, to SU(3) quenched configurations by a monopole
creation operator. The low-lying eigenvalues of the Overlap Dirac operator are
computed from the gauge links of the normal configurations and the
configurations with additional monopoles. Next, we compare the distributions of
the nearest-neighbor spacing of the low-lying eigenvalues with the prediction
of the random matrix theory. The low-lying eigenvalues not depending on the
scale parameter $\Sigma$ are compared to the prediction of the random matrix
theory. The results show the consistency with the random matrix theory. Thus,
the additional monopoles do not affect the low-lying eigenvalues. Moreover, we
discover that the additional monopoles increase the scale parameter $\Sigma$.
We then evaluate the chiral condensate in the $\overline{\mbox{MS}}$ scheme at
2 [GeV] from the scale parameter $\Sigma$ and the renormalization constant
$Z_{S}$. The final results clearly show that the chiral condensate linearly
decreases by increasing the monopole charges.
