“…The wavefront of the probe beam is slightly distorted when it propagates through the illuminated volume of the liquid sample. This distortion can be expressed with an additional phase shift to the probe beam by Uðr; tÞ ¼ ð2p=k p ÞL ½nðr; tÞ À nð0; tÞ [22,23], where nðr; tÞ ¼ n 0 þ ðdn=dTÞTðr; tÞ þ ðdn=dCÞCðr; tÞ, n 0 is the refractive index, L is the sample thickness, dn=dT and dn=dC are the refractive index temperature and concentration coefficients, respectively, at the probe beam wavelength k p . The phase shift can be written in terms of Uðr; tÞ ¼ h T ½Tðr; tÞ À Tð0; tÞ þ h c ½Cðr; tÞ À Cð0; tÞ, with h T ¼ ð2p=k p Þ Lðdn=dTÞ and h c ¼ ð2p=k p ÞLðdn=dCÞ.…”