We present a high-resolution electron microscopy study of the microstructure of boron nitride thin films grown on silicon ͑100͒ by radio-frequency plasma-assisted chemical vapor deposition using B 2 H 6 ͑1% in H 2 ͒ and NH 3 gases. Well-adhered boron nitride films grown on the grounded electrode show a highly oriented hexagonal structure with the c-axis parallel to the substrate surface throughout the film, without any interfacial amorphous layer. We ascribed this textured growth to an etching effect of atomic hydrogen present in the gas discharge. In contrast, films grown on the powered electrode, with compressive stress induced by ion bombardment, show a multilayered structure as observed by other authors, composed of an amorphous layer, a hexagonal layer with the c-axis parallel to the substrate surface and another layer oriented at random. © 1996 American Institute of Physics. ͓S0021-8979͑96͒04422-2͔In recent years, an important research activity has been directed to the preparation of boron nitride ͑BN͒ thin films by several low-pressure physical vapor deposition ͑PVD͒ and chemical vapor deposition ͑CVD͒ methods, to be used as protective coatings and as dielectric layers in many optical, mechanical, and electronic applications. [1][2][3] This is due to the outstanding properties of BN, such as optical transparency, chemical inertness, hardness, high electrical resistivity, high thermal conductivity, and low dielectric losses. In thin film form, BN can crystallize in various phases depending on preparation conditions. Among them are the hexagonal ͑h-BN͒ structure, similar to that of graphite but insulating, the cubic ͑c-BN͒ structure analogous to that of diamond, and an amorphous ͑a-BN͒ structure. Successful deposition techniques of c-BN, considered as a promising material for tribological and high-temperature electronics applications, all make use of ion bombardment during deposition, thought to be an essential condition. However, this involves a high compressive stress, which limits the film thickness and often leads to poor adherence or even cracking and delamination. 4 Such problems do not occur in the case of noncubic BN, believed a good candidate dielectric material for sub-halfmicron microelectronics technology. 5 Since the work of Kester et al.,6 several researchers have reported cross-sectional high-resolution transmission electron microscopy ͑HRTEM͒ studies of the structure of BN films obtained by ion beam-assisted PVD methods 7-10 and radio frequency ͑rf͒ bias magnetron sputtering. 11 These studies revealed a multilayered structure of the films, composed of an initial few-nanometer-thick a-BN layer next to the Si substrate, followed by an h-BN layer with the c-axis parallel to the substrate surface, and finally by a c-BN layer. The preferred orientation of the intermediate h-BN layer is thought to be a result of the increasing biaxial compressive stress in the film, induced by ion bombardment. 12 Without bias or ion assistance, it has been shown that the hexagonal layer grows with the c-axis norma...