Advances in multichannel ellipsometric techniques for in-situ and real-time characterization of thin films

Recent advances in the design of multichannel ellipsometers based on rotating-element principles have significantly increased their power for applications involving in-situ, real-time analysis of thin films and surfaces. These advances include: (i) extensions in the upper spectral limit beyond the typical value of 4.5 eV, and (ii) increases in the number of extracted parameters beyond the usual two, namely the ellipsometric angles (ψ, Δ). An extended spectral range is enabled, for example, by use of a tandem light source configuration and a grating spectrograph having two stages of order-sorting filters mounted over the window of the linear array detector. With an upper spectral limit of 6.5 eV, such ellipsometers are particularly useful in growth analysis for wide band gap thin films. The larger parameter set is enabled by use of dual or single rotating compensators for polarization state modulation and/or analysis, replacing the traditional rotating polarizer. For the single rotating-compensator instrument in the PSCrA configuration, one can extract the Stokes vector of the reflected beam, and thus its degree of polarization. This in turn can provide information on sample thickness variations over the beam cross-section and can suppress the effects of multiply-scattered light so that non-uniform and macroscopically rough surfaces can be analyzed. For the dual rotating compensator in the PCr1SCr2A configuration, one can extract the entire Mueller matrix of the sample and thus the characteristics of anisotropic surfaces and thin films. Applications of these advances include studies of thickness evolution of the phase for boron nitride and silicon film growth, and the nature and origin of surface-induced optical anisotropy of (110) silicon.

[1]  D. Medlin,et al.  Review of advances in cubic boron nitride film synthesis , 1997 .

[2]  R. Collins,et al.  Multichannel mueller matrix ellipsometry for simultaneous real-time measurement of bulk isotropic and surface anisotropic complex dielectric functions of semiconductors. , 2003, Physical review letters.

[3]  David E. Aspnes,et al.  Minimal-data approaches for determining outer-layer dielectric responses of films from kinetic reflectometric and ellipsometric measurements , 1993 .

[4]  D. Aspnes Precision bounds to ellipsometer systems. , 1975, Applied optics.

[5]  Hiroyuki Fujiwara,et al.  Optimization of hydrogenated amorphous silicon p–i–n solar cells with two-step i layers guided by real-time spectroscopic ellipsometry , 1998 .

[6]  Jon Opsal,et al.  Analytic representations of the dielectric functions of materials for device and structural modeling , 1998 .

[7]  R. Collins,et al.  Analysis of specular and textured SnO2:F films by high speed four-parameter Stokes vector spectroscopy , 1999 .

[8]  D. Aspnes New developments in spectroellipsometry : the challenge of surfaces , 1993 .

[9]  Joungchel Lee,et al.  Dual rotating-compensator multichannel ellipsometer: Instrument development for high-speed Mueller matrix spectroscopy of surfaces and thin films , 2001 .

[10]  J. Zapien,et al.  Characterization of cubic boron nitride growth using UV-extended real-time spectroscopic ellipsometry: Effect of plasma additions and dynamic substrate bias steps , 2002 .

[11]  H. Nguyen,et al.  In situ determination of dielectric functions and optical gap of ultrathin amorphous silicon by real time spectroscopic ellipsometry , 1991 .

[12]  Robert W. Collins,et al.  Automatic rotating element ellipsometers: Calibration, operation, and real‐time applications , 1990 .

[13]  R. Collins,et al.  Alignment and calibration of the MgF2 biplate compensator for applications in rotating-compensator multichannel ellipsometry. , 2001, Journal of the Optical Society of America. A, Optics, image science, and vision.

[14]  A. A. Studna,et al.  High precision scanning ellipsometer. , 1975, Applied optics.

[15]  J. Zapien,et al.  Multichannel ellipsometer for real time spectroscopy of thin film deposition from 1.5 to 6.5 eV , 2000 .

[16]  Ilsin An,et al.  Rotating-compensator multichannel ellipsometry: Applications for real time Stokes vector spectroscopy of thin film growth , 1998 .

[17]  J. Zapien,et al.  Calibration and data reduction for a UV-extended rotating-compensator multichannel ellipsometer , 2004 .

[18]  R. Collins,et al.  Rotating-compensator multichannel ellipsometry for characterization of the evolution of nonuniformities in diamond thin-film growth , 1998 .

[19]  A. Matsuda,et al.  INTERFACE-LAYER FORMATION MECHANISM IN A-SI:H THIN-FILM GROWTH STUDIED BY REAL-TIME SPECTROSCOPIC ELLIPSOMETRY AND INFRARED SPECTROSCOPY , 1999 .

[20]  Optical depth profiling of band gap engineered interfaces in amorphous silicon solar cells at monolayer resolution , 1998 .

[21]  Bernd Rech,et al.  Intrinsic microcrystalline silicon: A new material for photovoltaics , 2000 .

[22]  R. Azzam,et al.  Photopolarimetric measurement of the Mueller matrix by Fourier analysis of a single detected signal. , 1978, Optics letters.

[23]  P. S. Hauge,et al.  Mueller matrix ellipsometry with imperfect compensators , 1978 .

[24]  G. L. Trigg,et al.  Encyclopedia of Applied Physics , 1994 .

[25]  Joshua M. Pearce,et al.  Evolution of microstructure and phase in amorphous, protocrystalline, and microcrystalline silicon studied by real time spectroscopic ellipsometry , 2003 .

[26]  L. Florez,et al.  Relationship among reflectance‐difference spectroscopy, surface photoabsorption, and spectroellipsometry , 1993 .

[27]  Russell Messier,et al.  Ultraviolet-extended real-time spectroscopic ellipsometry for characterization of phase evolution in BN thin films , 2001 .