An amorphous mixing layer (3.5–4.0 nm in thickness) containing silicon (Si), oxygen (O), molybdenum (Mo) atoms, named
α-SiO
x(Mo), is usually formed by evaporating molybdenum trioxide (MoO
3) powder on an n-type Si substrate. In order to investigate the process of adsorption, diffusion and nucleation of MoO
3 in the evaporation process and ascertain the formation mechanism of
α-SiO
x(Mo) on a atomic scale, the first principle calculation is used and all the results are obtained by using the Vienna
ab initio simulation package. The possible adsorption model of MoO
3 on the Si (100) and the defect formation energy for substitutional defects and vacancy defects in
α-SiO
2 and
α-MoO
3 are calculated by the density functional theory. The results show that an amorphous layer is formed between MoO
3 film and Si (100) substrate according to
ab initio molecular dynamics at 1500 K, which are in good agreement with experimental observations. The O and Mo atoms diffuse into Si substrate and form the bonds of Si—O or Si—O—Mo, and finally, form an
α-SiO
x(Mo) layer. The adsorption site of MoO
3 on the reconstructed Si (100) surface, where the two oxygen atoms of MoO
3 bond with two silicon atoms of Si (100) surface, is the most stable and the adsorption energy is -5.36 eV, accompanied by the electrons transport from Si to O. After the adsorption of MoO
3 on the Si substrate, the structure of MoO
3 is changed. Two Mo—O bond lengths of MoO
3 are 1.95 Å and 1.94 Å, respectively, elongated by 0.22 Å and 0.21 Å compared with the those before the adsorption of MoO
3 on Si substrate, while the last bond length of MoO
3 is little changed. The defect formation energy value of neutral oxygen vacancy in
α-SiO
2 is 5.11 eV and the defect formation energy values of neutral oxygen vacancy in
α-MoO
3 are 0.96 eV, 1.96 eV and 3.19 eV, respectively. So it is easier to form oxygen vacancy in MoO
3 than in SiO
2, which implies that the oxygen atoms will migrate from MoO
3 to SiO
2 and forms a 3.5–4.0-nm-thick
α-SiO
x(Mo) layer. As for the substitutional defects in MoO
3 and SiO
2, Mo substitutional defects are most likely to form in SiO
2 in a large range of Mo chemical potential. So based on our obtained results, the forming process of the amorphous mixing layer may be as follows: the O atoms from MoO
3 bond with Si atoms first and form the SiO
x. Then, part of Mo atoms are likely to replace Si atoms in SiO
x. Finally, the ultra-thin buffer layer containing Si, O, Mo atoms is formed at the interface of MoO
3/Si. This work simulates the reaction of MoO
3/Si interface and makes clear the interfacial geometry. It is good for us to further understand the process of adsorption and diffusion of atoms during evaporating, and it also provides a theoretical explanation for the experimental phenomenon and conduces to obtaining better interface passivation and high conversion efficiency of solar cell.