Using surface laser light scattering spectroscopy, we have observed for the first time the crossover from capillary to Rayleigh (elastic) surface fluctuations on polymer solutions. At low polymer concentrations c c* the capillary mode evolves into a Rayleigh mode. The surface laser light scattering data is quantitatively discussed within the context of recent theory.The surface tension [l] and bulk hydrodynamics [2] of polymer solutions have been the subject of extensive recent study. However, their surface hydrodynamics has received only scant attention [3][4][5][6][7]. The anomalous damping of capillary waves due to the frequency dependence of the bulk viscosity has been probed both for rigid rod solutions (carboxymethyl cellulose in water [5]) and for semidilute flexible polymer solutions (polystyrene in ethylmethylcetone [6] and polyisobutylene in decane [7]). However, surface Rayleigh waves, driven by the (visco)-elasticity of the underlying bulk solutions, have never been observed.Early theoretical treatments of polymer surface modes modeled the bulk material as a single-component viscoelastic fluid [3], which approach assumes a constitutive equation. By contrast, the coupled two-component fluid theory [4] deduces an appropriate constitutive equation in order to study the surface modes on entangled polymer solutions. These authors argue for a crossover from capillary (surface tension) to Rayleigh (surface elastic) modes as a function of polymer concentration. At low polymer concentration, the surface restoring force is dominated by the solvent surface tension; the surface fluctuation is a capillary mode with dispersion relation co -q 3 ' 2 . At high polymer concentration, the restoring force is enhanced, being dominated by the elasticity of the polymer entanglements (which elasticity increases with polymer concentration); the surface fluctuation is a Rayleigh mode with dispersion relation co -q. In this Letter, we report the first observations, using surface laser light scattering (SLLS) spectroscopy, of this crossover with polymer concentration from capillary to Rayleigh waves on the surfaces of polymer solutions.