Structure and hydrogen content of polymorphous silicon thin films studied by spectroscopic ellipsometry and nuclear measurements

The dielectric functions of amorphous and polymorphous silicon films prepared under various plasma conditions have been deduced from UV-visible spectroscopic ellipsometry measurements. The measured spectra have been firstsimulated by the use of the Tauc-Lorentz dispersion model and then the compositions of the films have been obtained by the use of the tetrahedron model combined with the Bruggeman effective medium approximation. This approach allows us to determine the hydrogen content, the crystalline fraction, and the void fraction of the films. This is particularly important in the case of polymorphous films in which the low crystalline fraction (below 10%) can only be detected when an accurate description of the effects of hydrogen on the dielectric function through the tetrahedron model is considered. The hydrogen content and film porosity deduced from the analysis of the spectroscopic ellipsometry measurements are in excellent agreement with the hydrogen content and film density deduced from combined elastic recoil detection analysis and Rutherford backscattering spectroscopy measurements. Moreover, despite their high hydrogen content (∼15%-20%) with respect to hydrogenated amorphous silicon films deposited at the same temperature (8%), polymorphous silicon films have a high density, which is related to their very low void fraction.

[1]  Eray S. Aydil,et al.  Mechanism of hydrogen-induced crystallization of amorphous silicon , 2002, Nature.

[2]  Collins,et al.  Finite-size effects on the optical functions of silicon microcrystallites: A real-time spectroscopic ellipsometry study. , 1993, Physical review. B, Condensed matter.

[3]  John R Abelson,et al.  The interaction of atomic hydrogen with very thin amorphous hydrogenated silicon films analyzed using in situ real time infrared spectroscopy: Reaction rates and the formation of hydrogen platelets , 1998 .

[4]  Regis Vanderhaghen,et al.  In situ investigation of polymorphous silicon deposition , 2000 .

[5]  D. Aspnes,et al.  Spectroscopic Analysis of the Interface Between Si and Its Thermally Grown Oxide , 1980 .

[6]  G. Jellison,et al.  Parameterization of the optical functions of amorphous materials in the interband region , 1996 .

[7]  J. Abelson,et al.  Absence of an abrupt phase change from polycrystalline to amorphous in silicon with deposition temperature. , 2001, Physical review letters.

[8]  P. Cabarrocas,et al.  Role of mobile hydrogen in the amorphous silicon recrystallization , 1995 .

[9]  Structural properties depicted by optical measurements in hydrogenated polymorphous silicon , 1999 .

[10]  O. Marty,et al.  Structural properties and recombination processes in hydrogenated polymorphous silicon , 2003 .

[11]  D. A. G. Bruggeman Berechnung verschiedener physikalischer Konstanten von heterogenen Substanzen. I. Dielektrizitätskonstanten und Leitfähigkeiten der Mischkörper aus isotropen Substanzen , 1935 .

[12]  Dc Daan Schram,et al.  On the effect of substrate temperature on a-Si:H deposition using an expanding thermal plasma , 1996 .

[13]  B. Schröder,et al.  Density of glow discharge amorphous silicon films determined by spectroscopic ellipsometry , 1994 .

[14]  B. Drévillon,et al.  Phase modulated ellipsometry from the ultraviolet to the infrared: In situ application to the growth of semiconductors , 1993 .

[15]  Smith,et al.  Optical constants of a series of amorphous hydrogenated silicon-carbon alloy films: Dependence of optical response on film microstructure and evidence for homogeneous chemical ordering. , 1987, Physical review. B, Condensed matter.

[16]  P. Roca i Cabarrocas,et al.  Plasma enhanced chemical vapor deposition of amorphous, polymorphous and microcrystalline silicon films , 2000 .

[17]  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.

[18]  Rj René Severens,et al.  An Expanding Thermal Plasma for Deposition of a-Si:H , 1995 .

[19]  Enric Bertran,et al.  Nanoparticle formation in low-pressure silane plasmas: bridging the gap between a-Si:H and μc-Si films , 1998 .

[20]  Y. Poissant,et al.  Plasma production of nanocrystalline silicon particles and polymorphous silicon thin films for large-area electronic devices , 2002 .

[21]  Jean-Paul Kleider,et al.  Midgap density of states in hydrogenated polymorphous silicon , 1999 .

[22]  Jean-Paul Kleider,et al.  Very low densities of localized states at the Fermi level in hydrogenated polymorphous silicon from capacitance and space-charge-limited current measurements , 1999 .

[23]  Feng,et al.  Dielectric functions and electronic band states of a-Si and a-Si:H. , 1992, Physical review. B, Condensed matter.

[24]  A. V. Kharchenko,et al.  Structural, optical, and electronic properties of hydrogenated polymorphous silicon films deposited from silane–hydrogen and silane–helium mixtures , 2003 .

[25]  P. Cabarrocas,et al.  Ion bombardment effects on microcrystalline silicon growth mechanisms and on the film properties , 2003 .

[26]  P. Roca i Cabarrocas,et al.  Shedding light on the growth of amorphous, polymorphous, protocrystalline and microcrystalline silicon thin films , 2001 .

[27]  Robert W. Collins,et al.  EVOLUTIONARY PHASE DIAGRAMS FOR PLASMA-ENHANCED CHEMICAL VAPOR DEPOSITION OF SILICON THIN FILMS FROM HYDROGEN-DILUTED SILANE , 1999 .

[28]  M. Vaněček,et al.  Thermally induced metastable defect studies on hydrogenated amorphous silicon films with different hydrogen contents , 1995 .

[29]  P. Cabarrocas,et al.  Etching and hydrogen diffusion mechanisms during a hydrogen plasma treatment of silicon thin films , 2002 .

[30]  Direct imaging of submicron-scale defect-induced birefringence in SrTiO3 bicrystals , 1998, cond-mat/9802058.

[31]  A. C. Adams,et al.  Optical properties of low‐pressure chemically vapor deposited silicon over the energy range 3.0–6.0 eV , 1981 .

[32]  P. Cabarrocas,et al.  Structure of plasma-deposited polymorphous silicon , 2002 .

[33]  P. Cabarrocas Plasma enhanced chemical vapor deposition of silicon thin films for large area electronics , 2002 .