Background: Reaction cross sections σR are available as a function of incident energy Ein for p scattering on a 208 Pb target. Very lately, we reanalyzed interaction cross sections σI (≈ σR)) for 42−51 Ca+ 12 C scattering at Ein = 280 MeV per nucleon, using the chiral (Kyushu) g-matrix folding model with the densities calculated with Gongny-HFB (GHFB) with and without the angular momentum projection (AMP). We determined neutron skin r skin and proton, neutron, matter radii, rp, rn, rm for the σI, using the Kyushu g-matrix folding model. One of the results is r 48 skin = 0.164 fm for 48 Ca. Aim: We determine r 208 skin from the central values of measured σR for p+ 208 Pb scattering, using the Kyushu g-matrix folding model with the GHFB+AMP densities. Results: The Kyushu g-matrix folding model with the GHFB+AMP densities reproduces σR in 40 ≤ Ein ≤ 180 MeV in one-σ level. The rm(AMP) calculated with GHFB+AMP slightly overestimates the lower bound 5.54 fm of rm(PREX) by 0.3%. We then identify the σR(AMP) with the lower bound of σR(PREX). The rp(PREX) and rn(PREX) in PREX are most reliable. The rp(AMP) and rn(AMP) slightly underestimate the central value rp(PREX) =5.45 fm by 0.1% and the central value rn(PREX) =5.78 fm by 3.6%, respectively. The small deviation allows us to scale the GHFB+AMP densities to the central values of rp(PREX) and rn(PREX). The Kyushu g-matrix folding model with the scaled densities almost reproduces the central values of σR when Ein = 40 − 81 MeV, so that both the σR(AMP) and σR(PREX) are in one σ of σR there. In Ein = 40 − 81 MeV, we determine the rm from the central values of σR and take the average for the rm. The averaged value is rm = 5.61 fm, leading to r 208 skin = 0.25 fm.