Measured differential cross sections for the scattering of 104 MeV ~ particles from 2~ and 28Si are analyzed on the basis of a deformed folding model. Rms-radii and values of the deformation parameters for the nuclear density distributions are extracted, and the effect of the size of the c~ particle is demonstrated. Previous discrepancies between (p, p') and (~, 0d) results are partly removed.It has been found that the real part U R (G) of the optical potential for the elastic a-nucleus scattering can be related to the nuclear density distribution p (r) by the equation [1,2,3] U,(r~) = S p(r) Vefr (r-G) d3 r.(1) An effective a-particle-bound nucleon interaction of a simple gaussian formis found to be quite satisfactory and was derived (as approximate result) [4,5] by folding the ~ particle form factor with a nucleon-nucleon interaction which fits the low energy data. According to Bernstein [3] the value of Vo = -37 MeV and the range p = 2.0 fm. The energy dependent constant 2R(E,) takes into account of deviations of the strength from the derived zero-energy a-nucleon scattering value Vo. The factor 2R may by determined empirically thus absorbing some uncertainties in the choice of Ve~. By fitting elastic a particle scattering to 4~ ,~R=0.815 was obtained at E, = 104 MeV [3]. This value proves to be a best value* throughout for the 104 MeV elastic a particle scattering [3,6]. Fortunately the scattering is rather insensitive to the detailed shape of the theoretically undefined imaginary potential [3]. Thus the imaginary potential Ux may be chosen proportional to the real part by introducing a further empirical * As pointed out in Ref.[5] Bernstein's value of V o is not correct. However, this is absorbed by the phenomenological value of JR"