Defect density and breakdown strength of single-layer thermal silicon oxides do not fulfill the requirements for dielectrics used in modern dynamic random access memory (DRAM) applications, 1-4 which require ultrathin dielectric films along with an increase of read/ write cycles and good charge retention capability. 5,6 Silicon oxidenitride-oxide (ONO) films constitute alternative dielectrics for nonconducting operation in DRAM cell capacitors, first reported by Watanabe et al. in 1984. 7 ONO structures exploit concomitantly the advantages of oxide and nitride films. 8 In ONO multilayer structures, the oxide in contact with the Si substrate (bottom oxide) provides device-quality electrical SiO 2 /Si interface. 6,9 The nitride layer increases the effective dielectric constant of the ONO sandwich 6 in such a way that a film twice as thick as SiO 2 -based dielectric shows equal capacitance, thus offering increased process reliability or, for comparable thickness, higher storage capacity. 10,11 Furthermore, the nitride layer acts as a diffusion barrier for boron transport from the doped poly-Si gate electrode toward the SiO 2 /Si interface. 8,12 The top oxide provides the electrical contact to the poly-Si gate electrode. 8,9 An ideal ONO structure could then provide 8 (i) low defect density, (ii) high effective dielectric constant, (iii) high electric breakdown strength, (iv) low current conduction, and (v) minimal B diffusion to the SiO 2 /Si interface. In order to achieve thinner dielectrics, as required for future DRAM applications, it is necessary to understand the properties of the ONO structure, something that cannot be achieved without precise knowledge of the composition through the film and how it is affected by the successive processing stages.Ultrathin ONO films are usually prepared 1,2,6,13,14 by thermal growth of a 2-5 nm thick SiO 2 film (bottom oxide) on Si substrates in dry oxygen. Subsequently a 5-10 nm thick Si 3 N 4 layer is deposited by a low pressure chemical vapor deposition (LPCVD) process. Finally, a thermal reoxidation is performed in wet or dry oxygen or, in order to form a top oxide without consuming any nitride, a LPCVD high temperature oxide can be deposited. Although this preparation route can be thought to produce a stacked ONO structure, it does not seem to do so, at least for ultrathin films. It was observed 6 that even very thin oxide layers of approximately 1 nm prevent electron-and hole-currents into the nitride very effectively. As this feature could not be explained by a simple model of a 1 nm oxide with sharp boundary between SiO 2 and Si 3 N 4 , it was assumed that thermal oxidation produced a graded transition between top oxide and nitride which removed Si 3 N 4 trap levels in the close vicinity of the Si 3 N 4 /SiO 2 interface. X-ray photoelectron spectroscopy (XPS) was used 15 to investigate the ONO structure obtained by the sequence: (i) thermal oxidation of Si at 900ЊC (90 Å bottom oxide), (ii) LPCVD nitride layer deposition (60-120 Å), and (iii) rapid thermal oxidation (...