Owing to a complex structure composed of carbidic Si-C and nitridic Si-N and C-N units, silicon carbonitride (SiCN) films display many unique properties. They are promising coating materials in advanced technology. Most recent reports [1][2][3][4][5][6] revealed many unique features of SiCN films which may be used as hard, dense, and high temperatureand corrosion-resistant coatings for metals (giving excellent tribological behavior), as well as highly selective gas separation membranes. [7] Of the various methods based on the gas-phase processes which are used for the formation of SiCN films, remote microwave plasma (RP)CVD from organosilicon precursors, developed in our laboratory, appeared to be a very useful technique, offering wellcontrolled deposition conditions free of film-damaging effects.[2]In this communication we report on the fabrication of amorphous SiCN films by RPCVD using hydrogen as an upstream gas for microwave plasma generation, and tris(dimethylamino)silane (TrDMAS), (Me 2 N) 3 SiH, as a novel single-source precursor, being a carrier of Si-N and C-N units. Owing to the presence of hydrosilyl, Si-H bonds in the TrDMAS molecule, this precursor is strongly reactive with hydrogen atoms fed from the plasma region to the CVD reactor. Moreover, the dimethylaminosilyl, Me 2 NSi, groups of the precursor may easily undergo a condensation reaction at elevated temperatures. The present study was undertaken in view of our earlier reports on the SiCN films produced by RPCVD from other aminosilane precursors, such as (dimethylamino)dimethylsilane, [8][9][10] Me 2 NSiHMe 2 , and bis(dimethylamino)methylsilane, [11,12] (Me 2 N) 2 SiHMe, which revealed their very promising useful properties. We describe the effect of substrate temperature on the growth rate, chemical structure, surface morphology, density, and photoluminescence of produced SiCN films. Figure 1 shows the effect of thermal activation on the kinetics of SiCN film growth from TrDMAS characterized by the substrate temperature, T S , dependency of the thickness-based film growth rate, r d , determined in the form of an Arrhenius plot. The decrease of r d with increasing T S (Fig. 1) and the negative value of the apparent activation energy E a ¼ À14 kJ mol À1 calculated from the slope of the Arrhenius plot, implies that film growth is mainly limited by the adsorption of film-forming precursors from the gas phase onto the growth surface. In this case, the apparent activation energy is expressed as E a ¼ E r þ DH ad , where E r denotes the activation energy of the film-forming reaction and DH ad is the apparent heat of adsorption of the film-forming precursors onto the growth surface and has a negative value, [13,14] thus the negative E a values are due to the fact that the absolute DH ad value is higher than the E r value.