Recently, Bozovic et al. reported that [Nature 536, 309-311 (2016)], in the overdoped side of the single-crystal 2− 4 (LSCO) films, the transition temperature and zero-temperature superfluid phase stiffness (0) will obey a two-class scaling law: = • √ (0) for ≤ and ∝ (0) for ≥ , where = (4.2 ± 0.5) 1 2 ⁄ , ≈ 15 , and ≈ 12 . They further pointed out that the parabolic scaling observed in the highly overdoped side indicates a quantum phase transition from a superconductor to a normal metal. In this paper, we propose a quantum partition function (QPF) for zero-temperature Cooper pairs, by which one can effectively distinguish the mean-field and quantum critical behaviors. We theoretically show that the two-class scaling law can be exactly derived by using the QPF, and the theoretical values of , , and are well in accordance with experimental measure values. Our analyses indicate that the linear scaling ∝ (0) is a mean-field behavior, while the parabolic scaling = • √ (0) is a quantum critical behavior. [1]. Y. J. Uemura et al., Universal Correlations between and * ⁄ (Carrier Density over Effective Mass) in High-Cuprate Superconductors, Phys. Rev. Lett. 62, 2317 (1989)