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.
Categories: hep-ph