I describe a mechanism to understand the relation between chiral-symmetry b
reaking and eigenmodes of the Dirac operator in lattice QCD with Kogut-Suss
kind sea quarks. It can be shown that if chiral symmetry is spontaneously b
roken, the eigenvalues lambda, should behave as z(i)/V for large volume V,
where z(i) is the i-th zero of the Bessel function. With neither chiral nor
lambda extrapolation, one can precisely calculate the chiral condensate us
ing only a small set of eigenvalues. Therefore, it is economical and free o
f systematic uncertainties. I present the first QCD data to support this me
chanism and encourage the lattice community to test and use it.