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We describe photon autocorrelation measurements of the Rayleigh linewidth in thin binary liquid films near the critical point. Measurements were made on four films of thickness 13.1, 4.1, 2.1, and 0.5 {μ}m. The films were formed by trapping and sealing samples of a 2,6-lutidine + water critical mixture between fused-silica optical flats. Dynamic scaling arguments predict that the Rayleigh linewidth dependence upon kξ for the films should be indistinguishable from that for otherwise identical large-volume samples, until conditions defined by both ξs/2 and Λs are satisfied. Here, s is the film thickness, ξ is the correlation length, and Λ≡2πk^-1 is the sampling length probed at wave number k. We find that, for the three thicker films to within 0.1 mK of their phase-separation temperatures and for the 0.5-{μ}m film to within 2 mK of an extrapolated critical temperature, our data agree with the predictions of renormalization-group theory for binary liquid mixtures in three spatial dimensions---with no adjustable parameters. No evidence of finite-size effects was seen, although both conditions are at least marginally satisfied for the 0.5-{μ}m film (Λs, and eight linewidths measured with ξ>s/2) and for the 2.1-{μ}m film (Λs/4, and fourteen linewidths measured with ξ>s/2). No effects were seen that could be traced to the presence of surface wetting layers. Finally, we observe a time- and film-thickness-dependent drift in the critical temperature which is not a critical phenomenon, and we find evidence for a noncritical phase transition in the thinnest film.
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Casalnuovo et al. (1984) studied this question.
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