On the nitrogen and oxygen incorporation in plasma-enhanced chemical vapor deposition (PECVD) SiOxNy films
Introduction
The plasma-enhanced chemical vapor deposition (PECVD) technique has been extensively utilized for the deposition of silicon-based dielectric films for applications as a passivating layer, a gate insulator in metal–oxide semiconductor structures and in optical devices [1], [2], [3], [4], [5], [6], [7], [8]. The fundamental advantage of this technique is that it enables control of the structural, mechanical and optical properties of the films deposited by adequately adjusting the deposition parameters [9], [10], [11], [12], [13], [14].
In particular, the utilization of SiO2 and SiOxNy films deposited by PECVD at low temperatures for optical device fabrication became very attractive due to the possibility of integrating the optical and electrical devices in the same chip [15], [16], [17]. At the same time, the advanced knowledge in the use of these materials in microelectronics could be easily applied to the integrated optics field [4], [7], [18], [19].
On the other hand, for application in optical devices, it is necessary to produce thicker films of approximately 3–4 μm. This makes the PECVD technique even more attractive due to the high deposition rates that can be attained with it [20], [21], [22], and which are not achievable by standard thermal-oxidation processes. In addition, thermally grown films exhibit high internal stress, which might produce cracking of the thicker films [21], [23]. Furthermore, the fact that the composition of the films can be controlled by the PECVD technique implies that films with different refractive index (n) can be deposited; this is a fundamental requirement for waveguide applications. However, due to the low temperatures and to the variety of reactions taking place in the plasma, undesirable SiOH and SiH bonds are present in the films [12], [24], [25], significantly increasing optical losses in the spectral region of interest in optical devices [26]. In the present work, we study deposition conditions that lead to an appropriate control of the refractive index, and at the same time prevent the incorporation of the undesirable SiOH and SiH bonds. Furthermore, a shift in the SiO stretching frequency, measured by IR absorption, with film thickness has been observed [27]. This parameter is associated with the angle of the SiOSi bridge, as well as with the material stoichiometry, which means that either the composition or the structure of the films is thickness-dependent; in this work, we also address this question.
The search for photoconducting and luminescent materials compatible with silicon-based integrated-circuit processing technology is another need for optoelectronic applications, and has received great attention in recent years [28], [29]. In this work, conditions that lead to silicon-rich material for photoluminescent and photoconducting applications are also investigated.
Section snippets
Experimental details
The SiOxNy films studied in this work were deposited in a standard 13.56-MHz RF PECVD capacitively coupled system described elsewhere [30], from appropriate gaseous mixtures of electronic grade (99.999%) silane (SiH4) and nitrous oxide (N2O).
Films with different nitrogen, silicon and oxygen content were obtained by varying the N2O/SiH4 flow ratio (R) and maintaining all other deposition conditions constant. Series of samples with similar thickness (∼100 nm) were grown with flow ratios ranging
Results
The infrared spectra for the set of thin samples (100 nm) deposited with varying N2O/SiH4 flow ratio are shown in Fig. 1. It should be mentioned that in Fig. 1, the 1500–4000-cm−1 spectral region was magnified three-fold, in order to appreciate better the NH and SiH bands. For high N2O/SiH4 flow ratio, the samples present a spectrum very similar to thermally grown SiO2, exhibiting only the characteristic SiO stretching, bending and rocking modes. As the flow ratio is decreased, nitrogen
Discussion
The FTIR results show that as the flow ratio is decreased, nitrogen concentration first increases, which becomes evident through SiN and NH FTIR absorption bands that continue to increase up to a value of R=1.5; for lower R, decreasing concentrations of NH bonds and increasing SiH bonds are observed. These must be accompanied by an increase in SiSi bonds, which is not evident from the FTIR results. However, the optical data and the RBS results are compatible with this hypothesis. For the
Conclusions
It was demonstrated that RF PECVD utilizing N2O/SiH4 mixtures as gaseous precursors leads to different material types, depending on the N2O/SiH4 flow ratio. For flow ratios in the range 5–2, a silicon dioxide-like oxynitride, SiOxNy with x+y=2 is obtained, and silicon-rich amorphous silicon-like oxynitride material for N2O/SiH4 flow ratios less than 2. The RBS results give strong evidence for the hypothesis that in the silicon dioxide-like films, N atoms enter into the network and substitute O
Acknowledgements
The authors acknowledge Ricardo Oliveira for help with sample characterization and Manfredo H. Tabacniks for the RBS measurements. The authors are also grateful to Brazilian agency FAPESP for financial support.
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2021, Solar Energy Materials and Solar CellsCitation Excerpt :Either by decreasing the gas flow rate of N2O or decreasing the gas flow rate of SiH4, SiHn becomes redundant and starts to combine with N and H radicals, which results in the formation of Si-N and Si-H bonds, even though less N2O leads to less N radicals [28]. On the other hand, increasing SiHn radicals can also lead to a high silicon concentration in the film, which results in a silicon rich SiOxNy film [28]. This can be confirmed by the Si-H peak shifts in Fig. 6b, which show the Si-H band shifting towards a lower wavenumber with decreasing N2O or increasing SiH4 [41].