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An alternative way to analyze quasi-elastic light scattering data for broadly distributed samples
Authors:C Wu
Institution:(1) Department of Chemistry, The Chinese University of Hong Kong, Shatin, N.T., Hong Kong
Abstract:In Quasi-Elastic Light Scattering (QELS), an apparent average hydrodynamic radius 
$$R_{h, app} \left( { \equiv  \left\langle {1/R_h } \right\rangle _z ]^{ - 1} } \right)$$
can be calculated from the measuredz-average translational diffusion coefficient langDrang z by using the Stokes-Einstein equation: 
$$R_{h, app}  = \frac{{k_B  T}}{{6\pi \eta \left\langle D \right\rangle _z }}$$
withk B,T and eegr being the Boltzmann constant, the absolute temperature and the solvent viscosity, respectively. It is known thatR h, app is not the same as langR h rang z because 
$$\frac{1}{{\left\langle D \right\rangle _z }} \ne \left\langle {\frac{1}{D}} \right\rangle _z$$
, especially when a sample is broadly distributed. In order to obtain langR h rang z instead ofR h, app, an alternative way to analyze QELS data is proposed: at first, we manipulate the measured correlation functionb 1/2|g (1)(t)| into a new function 
$$\int_t^\infty  {b^{1/2} } \left| g \right.^{(1)} (t)\left| {dt} \right.$$
; and then, we can analyze this new function to obtain an apparent parameter langDrangapp and an apparent distribution width 
$$\mu _{2, app} (D)/\left\langle D \right\rangle _{app}^2$$
. We have shown that no matter how broadly a sample is distributed, langDrangapp can be easily reduced to langR h rang z , and 
$$\mu _{2, app} (D)/\left\langle D \right\rangle _{app}^2$$
is directly related to the distribution width. In this report, besides using a simulated time correlation function, we also used two measured correlation functions of a latex dispersion with a broad particle size distibution and a polystyrene standard with a broad molecular weight distribution to demonstrate this alternative way.
Keywords:QELS  DLS  hydrodynamic size  polydispersity  data analysis
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