  Recently we have found that integral of the squared Coulomb wave function
describing systemcomposed of charged pion and central charged fragment
$Z_{eff}$ protons, $|\psi_r(r)|^2$, times pion source function $\rho(r)$ (of
the size $\beta$), $\intdr |\psi_r(r)|^2 \rho(r)$, shows a quasiscaling
behavior. This is approximately invariant under the following transformation:
$(\beta,Z_{eff}) \to (\lambda\beta,\lambda Z_{eff})$; $\lambda >0$. We called
such behavior $\beta-Z_{eff}$ quasiscaling. We examine this quasiscaling
behavior in detail. In particular we provide a semi-analytical examination of
this behavior and confirm it for the exponential pionic source functions in
addition to the Gaussian ones and for the production of K mesons as well. When
combined with the results of the HBT, a result of the yield ratio allows us to
estimate the size of the central charged fragment (CCF) to be $125\le
Z_{eff}\le 150$ for Pb+Pb collisions at energy 158 GeV/nucleon. From our
estimation, the baryon number density $0.024 \le n_{B}\le0.036$ [1/fm^3] is
obtained.
