“…When the β-AsP/SiC heterojunction absorbs enough energy under the irradiation of sunlight, the electron in the valence band of both β-AsP and SiC layers will be excited into the conduction band. Unlike type-II heterojunctions, 48,50,[58][59][60][61][62] the direction of the built-in electric field is from SiC to β-AsP, which is the most significant distinction between the two forms of heterojunctions, that is to say, due to the built-in electric field from SiC to β-AsP, the photogenerated electrons in the CBM of β-AsP will recombine with the photogenerated holes in the VBM of the SiC layer. Thus, the photogenerated electrons accumulate in the CBM of SiC layer and the photogenerated holes gather in the VBM of β-AsP layer, suggesting that the photogenerated carriers are effectively separated in different semiconductors.…”