Structural properties of microcrystalline silicon in the transition from highly crystalline to amorphous growth

Abstract The growth of microcrystalline silicon prepared by plasma-enhanced chemical vapour deposition depends on the deposition conditions and yields films with variable content of crystalline grains, amorphous network, grain boundaries and voids. The changes in the structural properties of a series of films grown under a variation of the dilution of the process gas silane in hydrogen, which induces a transition from highly crystalline to amorphous growth, were investigated. The evolution of the crystalline volume fraction was quantitatively analysed by Raman spectroscopy and X-ray diffraction. The results confirm the need for proper correction of the Raman data for optical absorption and Raman cross-section. Transmission electron microscopy was used to investigate the characteristics and the variation in the microstructure. Upon increasing the silane concentration the strong columnar growth with narrow grain boundaries degrades towards the growth of small irregularly shaped grains enclosed in an amorpho...

[1]  F. Finger,et al.  Structure and growth of hydrogenated microcrystalline silicon : investigation by transmission electron microscopy and Raman spectroscopy of films grown at different plasma excitation frequencies , 1997 .

[2]  É. Bustarret,et al.  Experimental determination of the nanocrystalline volume fraction in silicon thin films from Raman spectroscopy , 1988 .

[3]  R. Collins,et al.  In situ ellipsometry of thin‐film deposition: Implications for amorphous and microcrystalline Si growth , 1989 .

[4]  Hellmut Fritzsche,et al.  Amorphous silicon and related materials , 1989 .

[5]  C. Jeynes,et al.  Low-energy (2-5 keV) argon damage in silicon , 1986 .

[6]  S. C. Moss,et al.  Evidence of Voids Within the As-Deposited Structure of Glassy Silicon , 1969 .

[7]  C. Fortmann,et al.  Prospects for utilizing low temperature amorphous to crystalline phase transformation to define circuit elements; a new frontier for very large scale integrated technology , 1996 .

[8]  Veprek,et al.  Effect of grain boundaries on the Raman spectra, optical absorption, and elastic light scattering in nanometer-sized crystalline silicon. , 1987, Physical review. B, Condensed matter.

[9]  M. Heintze,et al.  Surface controlled plasma deposition and etching of silicon near the chemical equilibrium , 1993 .

[10]  R. Ewing,et al.  Image simulation of partially amorphous materials , 1993 .

[11]  J. Perrin Plasma and surface reactions during a-Si:H film growth , 1991 .

[12]  T. Akasaka,et al.  In situ real time studies of the formation of polycrystalline silicon films on glass grown by a layer‐by‐layer technique , 1995 .

[13]  S. A. Solin,et al.  Raman Spectrum of Wurtzite Silicon , 1973 .

[14]  Solomon,et al.  Real-time spectroscopic ellipsometry study of the growth of amorphous and microcrystalline silicon thin films prepared by alternating silicon deposition and hydrogen plasma treatment. , 1995, Physical review. B, Condensed matter.

[15]  T. C. Huang Surface and Ultra-Thin Film Characterization by Grazing-Incidence Asymmetric Bragg Diffraction , 1989 .

[16]  B. Drévillon,et al.  Role of Hydrogen Plasma during Growth of Hydrogenated Microcrystalline Silicon: In Situ UV-Visible and Infrared Ellipsometry Study , 1994 .

[17]  Reinhard Carius,et al.  Improvement of grain size and deposition rate of microcrystalline silicon by use of very high frequency glow discharge , 1994 .