Orientation-dependent stress relaxation in hetero-epitaxial 3C-SiC films

Residual stresses in epitaxial 3C-SiC films on silicon, for chosen growth conditions, appear determined by their growth orientation. Stress evaluation locally with Raman spectroscopy, and across a 150 mm wafer with curvature measurements, indicate that thin films can be grown on Si(100) with residual tensile stresses as low as 150 MPa. However, films on Si(111) retain a considerably higher stress, around 900 MPa, with only minor decrease versus film thickness. Stacking faults are indeed geometrically a less efficient relief mechanism for the biaxial strain of SiC films grown on Si(111) with 〈111〉 orientation. Residual stresses can be tuned by the epitaxial process temperatures.

[1]  K. Röll,et al.  Analysis of stress and strain distribution in thin films and substrates , 1976 .

[2]  S. Kawado,et al.  Stacking fault annihilation dependence on surface orientation in silicon , 1982 .

[3]  H. Matsunami,et al.  Surface morphology of cubic SiC(100) grown on Si(100) by chemical vapor deposition , 1986 .

[4]  Henry Guckel,et al.  Surface micromachined pressure transducers , 1991 .

[5]  I. Wolf Micro-Raman spectroscopy to study local mechanical stress in silicon integrated circuits , 1996 .

[6]  H. Nagasawa,et al.  3C-SiC single-crystal films grown on 6-inch Si substrates , 1997 .

[7]  L. Ley,et al.  Raman scattering in polycrystalline 3 C − SiC : Influence of stacking faults , 1998 .

[8]  Heteroepitaxial Growth of SiC on Si(100) and (111) by Chemical Vapor Deposition Using Trimethylsilane , 1999 .

[9]  M. Mehregany,et al.  Quantitative evaluation of biaxial strain in epitaxial 3C-SiC layers on Si(100) substrates by Raman spectroscopy , 2002 .

[10]  S. Öberg,et al.  Stacking faults in 3C-, 4H-, and 6H-SiC polytypes investigated by an ab initio supercell method , 2003 .

[11]  T. Page,et al.  The contact response of thin SiC-coated silicon systems—characterisation by nanoindentation , 2003 .

[12]  Interfacial strain in 3C‐SiC/Si(100) pseudo‐substrates for cubic nitride epitaxy , 2003 .

[13]  G. Ferro,et al.  Control of 3C–SiC/Si wafer bending by the “checker‐board” carbonization method , 2005 .

[14]  M. Capano,et al.  Residual strains in cubic silicon carbide measured by Raman spectroscopy correlated with x-ray diffraction and transmission electron microscopy , 2006 .

[15]  D. Chaussende,et al.  X-ray diffuse scattering from stacking faults in thick 3C-SiC single crystals , 2006 .

[16]  A. Leycuras,et al.  Stress relaxation during the growth of 3C-SiC∕Si thin films , 2006 .

[17]  M. Mehregany,et al.  The mechanical properties of polycrystalline 3C-SiC films grown on polysilicon substrates by atmospheric pressure chemical-vapor deposition , 2006 .

[18]  H. Nakanishi,et al.  Suppression of crack generation in GaN epitaxy on Si using cubic SiC as intermediate layers , 2006 .

[19]  O. Ambacher,et al.  Group III nitride and SiC based MEMS and NEMS: materials properties, technology and applications , 2007 .

[20]  Konstantin Vassilevski,et al.  Prospects for SiC electronics and sensors , 2008 .

[21]  S. Saddow,et al.  Residual Stress in CVD-grown 3C-SiC Films on Si Substrates , 2008 .

[22]  C. Zorman,et al.  Micro‐ and nanomechanical structures for silicon carbide MEMS and NEMS , 2008 .

[23]  A. Iacopi,et al.  Growth of 3C―SiC on 150-mm Si(100) substrates by alternating supply epitaxy at 1000 °C , 2011 .

[24]  C Locke,et al.  Advanced Residual Stress Analysis and FEM Simulation on Heteroepitaxial 3C–SiC for MEMS Application , 2011, Journal of Microelectromechanical Systems.