Abstract
With the aim of investigating the stability conditions of biaxial nematic liquid crystals, we
study the effect of adding a non-adsorbing ideal depletant on the phase behavior of colloidal
hard boardlike particles. We take into account the presence of the depletant by introducing an
effective depletion attraction between a pair of boardlike particles. At fixed depletant fugacity,
the stable liquid-crystal phase is determined through a mean-field theory with restricted
orientations. Interestingly, we predict that for slightly elongated boardlike particles a critical
depletant density exists, where the system undergoes a direct transition from an isotropic
liquid to a biaxial nematic phase. As a consequence, by tuning the depletant density, an easy
experimental control parameter, one can stabilize states of high biaxial nematic order even
when these states are unstable for pure systems of boardlike particles.
| Original language | English |
|---|---|
| Article number | 284128 |
| Pages (from-to) | 1-9 |
| Number of pages | 9 |
| Journal | Journal of Physics: Condensed Matter |
| Volume | 24 |
| DOIs | |
| Publication status | Published - 2012 |
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