“…39 Evanescent wave dynamic light scattering 10 combines the advantages of dynamic light scattering (DLS), i.e., statistical averaging and fast detection with a localized probing due to the short penetration depth, κ −1 , of an evanescent wave that is produced under total internal reflection conditions at an interface. 9 However, the interpretation of the measured intensity time autocorrelation function (TCF), g (2) (q, t; κ) = I (q, t; κ)I (q, 0; κ) / I (t) 2 , is far from trivial as it incorporates both confinement effects and the specific evanescent wave illumination that is decaying exponentially in space away from the solid-liquid interface. In the dilute limit, g (2) (q, t; κ) was originally calculated by Lan et al 10 taking into account the evanescent geometry and the wall mirror effect, while its initial decay incorporating the anisotropic viscous drag effect as a function of distance from the wall was more recently calculated by Holmqvist et al 14,28,40 With increasing volume fraction (φ), particle-particle HIs become important and modify the wall-induced drag effect.…”