As group III-nitride semiconductors are thinned to only a few atomic layers, regarding as 2D materials, it would lead to an ultrawide bandgap (E g ) due to the quantum confinement effect, [11,12] which can be used as ultraviolet optoelectronic devices needed ultrawide E g semiconductors. [13,14] Moreover, 2D group III-nitride semiconductors showing anomalously temperature-dependent thermal conductivity and orbitally driven ultra-low thermal conductivity have been predicted, [15,16] which make them prospective for applications in energy conversion, for example, thermos-electrics. [17] However, the experimental synthesis of 2D group III-nitride semiconductors is still meeting with tremendous difficulties due to the fact that group III-nitride semiconductors more easily orientate along c-axis than any other axis [18] and the lateral mobility for precursor atoms of group III-nitride materials, i.e., AlN, is very low, [19] which result in the formation of 3D crystal structure. Moreover, the surface energy constraint and large lattice mismatch between group III-nitride semiconductors and substrates would also lead to the formation of 3D island crystal. [11] In this work, we have successfully realized the epitaxial growth of 2D AlN layers sandwiched between graphene and Si substrates for the first time in the world by metal organic chemical vapor deposition (MOCVD). On the one hand, Si (111) surface with high symmetry [20] has stable adsorption sites for Al and N adatoms, Figure S1 in the Supporting Information. On the other hand, Si has a lattice mismatch with AlN(0001) of ≈19%, [21] Figure S2 in the Supporting Information, producing the tensile stress together with the effect of Gibbs free energy that drive the crystal structure of 2D AlN transforming from R3m structure to P6 3 MC structure. [22][23][24] During the growth process, hydrogenation for graphene/Si hetero-structures with hydrogen (H 2 ) guarantees the formation of 2D AlN layers. The 2D AlN layers are sandwiched between graphene and Si substrates after hydrogenation, while no interlayer can be found between graphene and Si substrates without hydrogenation. To further study the formation mechanism of 2D AlN layers and the effect of hydrogenation on the formation of 2D AlN layers, theoretical calculations with first-principles calculations based on density functional theory (DFT) have been carried out. We further predicted and determined the E g of the 2D AlN layers theoretically and experimentally by Hartree-Fock local density