  The PREX and the CREX group reported their skin values. Using the Love-Franey
(LF) $t$-matrix folding model with the neutron and proton densities scaled to
the neutron radius $r_{\rm n}^{208}({\rm PREX2})$ and the proton radius of the
electron scattering, we found that the model reproduces $\sigma_R$ for p+
$^{208}$Pb scattering at $E_{\rm lab} = 534.1, 549, 806$MeV. Zenihiro {\it el
al. } deduce neutron radii $r_{\rm n}^{48,40}({\rm exp})$ from proton elastic
scattering, whereas we determine $r_{\rm m}^{\rm 40}({\rm exp})=3.361 \pm
0.075$fm from measured $\sigma_R$ for $^{4}$He+ $^{40}$Ca scattering. Our first
aim is to determine $r_{\rm skin}^{\rm 208}$ from measured $\sigma_R$ of
p+$^{208}$Pb scattering at $E_{\rm lab} = 534.1, 549, 806$MeV by using the LF
$t$-matrix folding model. Our second aim is to determine $r_{\rm skin}^{\rm
48}$ from the $r_{\rm m}^{\rm 40}({\rm exp})$ and $\Delta \equiv r_{\rm m}^{\rm
48}({\rm exp})-r_{\rm m}^{\rm 40}({\rm exp})$ that is evaluated from the
$r_{\rm n}^{48,40}({\rm exp})$ and the $r_{\rm p}^{48,40}({\rm exp})$
calculated with the isotope shift method based on the electron scattering. For
the first aim, we use the LF $t$-matrix model with the densities scaled from
the D1S-GHFB+AMP neutron density. The D1M-GHFB+AMP is used to estimate a
theoretical error. The resulting skin values are $r_{\rm skin}^{\rm 208}= 0.324
\pm 0.047$fm for D1S and $r_{\rm skin}^{\rm 208}({\rm exp})=0.333 \pm 0.047 $fm
for D1M. The $\Delta=0.109$fm and $r_{\rm m}^{\rm 40}({\rm exp})=3.361 \pm
0.075$fm yield $r_{\rm m}^{\rm 48}=3.470 \pm 0.075$fm, leading to $r_{\rm
skin}^{\rm 48}=0.144 \pm 0.075$fm. We conclude that $r_{\rm skin}^{208}({\rm
exp})=0.324 \pm (0.047)_{\rm exp} \pm (0.009)_{\rm th}~{\rm fm}$ for p
scattering at $E_{\rm lab} = 534.1, 549, 806$MeV. Our skin values are
consistent with the PREX2 and CREX values.
