Thick SiOxNy and SiO2 films obtained by PECVD technique at low temperatures

In this work we present the results on the fabrication of thick silicon oxynitride and dioxide films deposited by conventional r.f. direct plasma enhanced chemical vapor deposition (DPECVD), at temperature as low as 320°C and from (N2O+SiH4) gaseous mixtures. The samples were characterized by profile measurements, ellipsometry measurements, etching rate, Fourier transform infrared spectroscopy (FTIR), and by scanning electron microscopy (SEM). The results show that for appropriate N2O/SiH4 flow ratio and SiH4 flow, it is possible to obtain very thick SiO2 and SiOxNy films (up to ∼10 μm) at high deposition rates (∼3 μm/h) and preserving the compositional and structural properties of similar high quality thin films obtained in a previous work (I. Pereyra, M.I. Alayo, J. Non-Cryst. Solids 212 (1997) 225). These thick SiO2 and SiOxNy films, exhibit a very well controlled refractive index, in a short range between ∼1.43 and ∼1.53, which is very attractive to SiO2/SiOxNy based waveguide fabrication. Besides the large thickness, the results show that the films present an etching rate just twice the thermally grown SiO2 rate, therefore lower than the reported values for PECVD SiO2 by other authors (M.S. Haque, H.A. Naseem, W.D. Brown, J. Electrochem. Soc. 142 (1995) 3864). Also etching experiments were performed using reactive ion etching (RIE) equipment on thick silicon oxynitride film grown onto silicon substrates covered by a thick DPECVD SiO2 buffer layer, in order to simulate a waveguide structure (ridge type) fabrication. The results of these tests show that it is possible to define vertical walls in these thick SiOxNy films, which is very important for ridge type waveguides.

[1]  Anthony J. Kenyon,et al.  OPTICAL-PROPERTIES OF PECVD ERBIUM-DOPED SILICON-RICH SILICA - EVIDENCE FOR ENERGY-TRANSFER BETWEEN SILICON MICROCLUSTERS AND ERBIUM IONS , 1994 .

[2]  H. Toba,et al.  Silica-based single-mode waveguides on silicon and their application to guided-wave optical interferometers , 1988 .

[3]  D. Flamm WITHDRAWN: Introduction to Plasma Chemistry , 1989 .

[4]  W. Brown,et al.  The Effects of Moisture on Strain Relief of Si‒O Bonds in Plasma‐Enhanced Chemical Vapor Deposited Silicon Dioxide Films , 1997 .

[5]  Dan Xu,et al.  Effect of power on interface and electrical properties of SiO2 films produced by plasma‐enhanced chemical‐vapor deposition , 1995 .

[6]  David V. Tsu,et al.  Atomic structure in SiO2 thin films deposited by remote plasma‐enhanced chemical vapor deposition , 1989 .

[7]  G. Lucovsky,et al.  Effect of rf power on remote-plasma deposited SiO2 films , 1993 .

[8]  G. Lucovsky,et al.  Thermal stabilization of device quality films deposited at low temperatures , 1990 .

[9]  B. Tweed,et al.  Fabrication of waveguides using low‐temperature plasma processing techniques , 1993 .

[10]  Donald L. Smith,et al.  Chemistry of SiO2 Plasma Deposition , 1993 .

[11]  David V. Tsu,et al.  Plasma enhanced chemical vapor deposition: Differences between direct and remote plasma excitation , 1987 .

[12]  M. I. Alayo,et al.  High quality low temperature DPECVD silicon dioxide , 1997 .

[13]  W. Brown,et al.  Characterization of High Rate Deposited PECVD Silicon Dioxide Films for MCM Applications , 1995 .

[14]  G. Lucovsky,et al.  Formation of device quality Si/SiO2 interfaces at low substrate temperatures by remote plasma enhanced chemical vapor deposition of SiO2 , 1990 .

[15]  I. Pereyra,et al.  Low temperature plasma enhanced chemical vapour deposition boron nitride , 1997 .