“…where K = 4π 2 n 2 (dn/dC) 2 /(N A λ 0 4 ) and q = (4πn/λ 0 ) sin(θ/2) with n, C, dn/dC, N A , and λ 0 being the refractive index, the concentration of the polymer solution, the specific refractive index increment, Avogadro's number, and the wavelength of light in a vacuum, respectively. The dn/dC value of polystyrene in THF is 0.186 mL/ g. 12,13 In dynamic LLS, 46 the Laplace inversion of each measured intensity−intensity time correlation function G (2) (q,t) in the selfbeating mode can result in a line-width distribution G(Γ). G(Γ) can be converted to a translational diffusion coefficient distribution G(D) or further to a hydrodynamic radius distribution f(R h ) via the Stokes− Einstein equation, R h = (k B T/6πη 0 )/D, where k B , T, and η 0 are the Boltzmann constant, the absolute temperature, and the solvent viscosity, respectively, by using both the cumulants and CONTIN analysis.…”