Dsp. Smith et al., NUMERICAL-ANALYSIS OF ELLIPSOMETRIC CRITICAL ADSORPTION DATA, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics, 55(1), 1997, pp. 620-636
A recent study [Dan S. P. Smith and Bruce M. Law, Phys. Rev. E 54, 272
7 (1996)] presented measurements of the ellipsometric coefficient at t
he Brewster angle <(rho)over bar> on the liquid-vapor surface of four
different binary liquid mixtures in the vicinity of their liquid-liqui
d critical point and analyzed the data analytically for large reduced
temperatures t. In the current report we analyze this (<(rho)over bar>
, t) data numerically over the entire range of t. Theoretical universa
l surface scaling functions P-+/-(x) from a Monte Carlo (MC) simulatio
n [M. Smock, H. W. Diehl, and D. P. Landau, Ber. Bunsenges. Phys. Chem
. 98, 486 (1994)] and a renormalization-group (RG) calculation [H. W.
Diehl and M. Smock, Phys. Rev. B 47, 5841 (1993); 48, 6470(E) (1993)]
are used in the numerical integration of Maxwell's equations to provid
e theoretical (<(rho)over bar>, t) curves that can be compared directl
y with the experimental data. While both the MC and RG curves are in q
ualitative agreement with the experimental data, the agreement is gene
rally found to be better for the MC curves. However, systematic discre
pancies are found in the quantitative comparison between the MC and ex
perimental (<(rho)over bar>, t) curves, and it is determined that thes
e discrepancies are too large to be due to experimental error. Finally
, it is demonstrated that <(rho)over bar> can be rescaled to produce a
n approximately universal ellipsometric curve as a function of the sin
gle variable xi(+/-)/lambda, where xi is the correlation length and la
mbda is the wavelength of light. The position of the maximum of this c
urve in the one-phase region, (xi(+)/lambda)(peak), is approximately a
universal number. It is determined that (xi(+)/lambda)(peak) is depen
dent primarily on the ratio c(+)/P-infinity,P-+ where P-+(x)congruent
to c(+x)(-beta/nu) for x much less than 1 and P-+(x)congruent to P(inf
inity,+)e(-x) for x much greater than 1. This enables the experimental
estimate of c(+)/P-infinity,P-+ = 0.90 +/- 0.24, which is significant
ly large compared to the MC and RG values of 0.577 and 0.442, respecti
vely.