I describe a mechanism to understand the relation between chiral-symmetry
breaking and eigenmodes of the Dirac operator in lattice QCD with
Kogut-Susskind sea quarks. It can be shown that if chiral symmetry is
spontaneously broken, the eigenvalues λi 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 λ extrapolation, one can precisely calculate the
chiral condensate using only a small set of eigenvalues. Therefore, it is
economical and free of systematic uncertainties. I present the first QCD data
to support this mechanism and encourage the lattice community to test and use
it.Comment: LATTICE98(confine