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A preliminary study of the liquid-glass transition phase diagram within the DLVO potential (see text) was given in this work. Equations (234) given there should respectively be replaced more correctly by Eqs. (212223) here. The latter equations are appropriate for a colloidal suspension. These changes, however, do not affect the numerical values for the idealized liquid-glass transition loci since the solidification equation remains unchanged (rigorous justification is given in Refs. c25 c27 c28 PLEEE8
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Here we follow the work of c27 for the definition of the memory function, which differs from those of c26 c25 by a factor [Formula Presented] [cf. Eq. (1.2) in c26 and Eq. (13) in c27]
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Here we follow the work of 27 for the definition of the memory function, which differs from those of 2625 by a factor D0q2 [cf. Eq. (1.2) in 26 and Eq. (13) in 27].
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