Field emission from single-, double-, and multi-walled carbon nanotubes chemically attached to silicon J. Appl. Phys. 111, 044326 (2012) Ceasing of voltage switching amongst graphitic shells in multiwalled carbon nanotubes: A route toward stability Appl. Phys. Lett. 100, 043505 (2012) Directly grown large area single-walled carbon nanotube films with very high sensitivity to normal pressure J. Appl. Phys. 111, 023502 (2012) Magnetoresistance of nanocarbon materials based on carbon nanotubes Low Temp. Phys. 37, 819 (2011) Characterization of the electrical contact between a conductive atomic force microscope cantilever and a carbon nanotube J. Appl. Phys. 110, 054305 (2011) Additional information on J. Appl. Phys. We report the optical property measurements on boron-doped diamond ͑BDD͒ films which were synthesized by microwave plasma-assisted chemical vapor deposition technique on Si ͑100͒ using methane in high hydrogen dilution and trimethylboron as precursors with varying boron concentration such that ͓B͔ / ͓C͔ gas = 100, 500, 1000, 2000, 4000, and 6467 ppm. These BDD films were investigated using a rotating analyzer variable angle spectroscopic ellipsometry ͑SE͒ from the near IR to UV range ͑830-193 nm͒. By applying the conventional Bruggeman effective medium approximation and linear regression analyses to the raw SE data that is, ͓ ͑ i ͒ , ⌬͑ i ͔͒ and pseudodielectric function ͑͗ r ͑ i ͒͘ , ͗ i ͑ i ͒͒͘, we determined the most appropriate model fit. The SE modeling was performed through the normal and point-by-point fit methods combined with the coupled and uncoupled bulk and surface layer approaches providing the details about the thin films' microstructure in terms of the ͑a͒ multilayer ͑component and surface͒ structure and component layer thickness of the films, ͑b͒volume fraction of constituents ͓f sp 3 C , f sp 2 C and void ͑f v ͒ in the component layer͔, ͑c͒ inhomogeneity of the structure along the growth axis and its variation with boron concentration, and ͑iv͒ surface roughness layer thickness ͑d s ͒ with dimensions less than the optical wavelength that is not otherwise available. A simplified three-layer structural model consisting of an interfacial layer, an intermediate ͑or bulk͒ layer, and a top surface roughness layer has been proposed, which simulates the ellipsometry data reasonably well with coupled point-by-point method. An estimator, i.e., mean squared error ͑ 2 ͒, is used to assess the accuracy of the model fit. The results ͑surface roughness and constituents' fraction͒ obtained through SE modeling are also compared with those from atomic force microscopy ͑AFM͒ and Raman spectroscopy to validate the layered model employed. Typically, high surface roughness values around 6 nm were found for films grown under different boron concentrations which is almost five times smaller than determined from AFM. In this context, we determined an approximate linear relationship between these two variables. The relatively smaller surface roughness for BDD films indicates the combined role of b...