We analyze the extended superfluid density data of Bo\v{z}ovi'{c} \textit{ et al}. taken on homogenous thin films to explore the critical properties of the thermal (TSM) and quantum superconductor to metal (QSM) transitions in overdoped LaSrCuO. The temperature dependence reveals remarkable agreement with d-wave BCS behavior, where $\sigma \propto 1/\lambda ^{2}$. No sign of the expected KTB transition is observable. We show that the critical amplitude scales as and with that as $T_{c}\propto \rho_{s}\left( 0\right) $, empirically verified by Bo\v{z}ovi'{c} \textit{et al}. Together with additional evidence for BCS behavior in overdoped LaSrCuO we show that the scaling relation $T_{c}\propto \lambda \left( 0\right) ^{-1}\propto \Delta \left( 0\right) \propto \xi \left( 0\right) ^{-1}\propto H_{c2}\left( 0\right) ^{-1/2}\propto \lambda_{0}^{-1}\propto \Delta_{0}\propto \xi_{0}^{-1}\propto H_{c20}^{-1/2}$ applies, by approaching the QSM and TSM transitions. This differs from the dirty limit behavior $\lambda \left( 0\right) \propto \xi \left( 0\right) ^{1/2}T_{c}\kappa =\lambda_{o}/\xi_{0}$, and puts a stringent constraint on the effect at work. We notice that potential candidates appear to be the nonlocal effects on the penetration depth of clean d-wave superconductors explored by Kosztin and Legget.

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