Complete breakdown of the Debye model of rotational relaxation near the isotropic-nematic phase boundary: Effects of intermolecular correlations in orientational dynamics
Prasanth P. Jose, Dwaipayan Chakrabarti, Biman Bagchi

TL;DR
This study investigates the failure of the Debye model of rotational relaxation near the isotropic-nematic phase boundary, revealing the role of intermolecular correlations and providing a mode coupling theory explanation.
Contribution
It demonstrates the breakdown of the Debye model in liquid crystals near the phase transition and links this to growing intermolecular correlations using simulations and mode coupling theory.
Findings
The ratio τ₁/τ₂ drops below one near the I-N transition.
The ratio τ₂/η exceeds hydrodynamic predictions near the transition.
The breakdown is due to increased orientational pair correlations.
Abstract
The Debye-Stokes-Einstein (DSE) model of rotational diffusion predicts that the rotational correlation times vary as , where is the rank of the orientational correlation function (given in terms of the Legendre polynomial of rank ). One often finds significant deviation from this prediction, in either direction. In supercooled molecular liquids where the ratio falls considerably below three (the Debye limit), one usually invokes a jump diffusion model to explain the approach of the ratio to unity. Here we show in a computer simulation study of a standard model system for thermotropic liquid crystals that this ratio becomes much less than unity as the isotropic-nematic phase boundary is approached from the isotropic side. Simultaneously, the ratio (where is the shear viscosity of the liquid)…
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