In 1910 Albert Einstein showed that the link between critical opalescence and Rayleigh scattering is quantitative.
2.
In 1908 the Polish physicist Marian Smoluchowski became the first to ascribe the phenomenon of critical opalescence to large density fluctuations.
3.
Under such an equilibrium assumption, in general, there are no macroscopically detectable critical states, which exhibit to the naked eye the phenomenon of critical opalescence.
4.
The line ends at the " chiral critical point ", marked by a star in this figure, which is a special temperature and density at which striking physical phenomena, analogous to critical opalescence, are expected . ( Reference for this section :, ).
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