Abstract
The coefficient of ellipticity of the liquid-vapor interface of liquid argon has been measured to be ρ¯×104=5.7±0.4 at 90°K, rising to 8.8±0.6 at 120°K. Assuming a Fermi density profile and isotropy of the dielectric constant in the interface region, this yields a 10%-90% interface thickness t(90°K)=7.9±0.5 Å and t(120°K)=15.2±1.0 Å, averaged over a surface dimension of the wavelength of light. The measurement is compared with predictions, and theoretical uncertainties are emphasised.