“…Each of these two in-plane motions are characterized by a frequency dependent elasticity modulus, ε (ω)=ε R (ω)+ε I (ω), where the first term is the real part or elasticity, and the second term is the imaginary or loss modulus, which is given by the product of the frequency, ω, and viscosity. In the case of polymer monolayers it has been clearly pointed out that the dilational elasticity and viscosity are orders of magnitude higher than the in-plane shear ones [13,14], thus one can safely neglect the contribution of the shear mode, and hereinafter we will write ε (ω)=ε(ω) +iωκ(ω), κ being the dilational viscosity.…”