# Orientational Phase Transitions and the Assembly of Viral Capsids

## TL;DR

This paper develops a generalized Landau-Brazovskii free energy model to analyze the complex orientational phase transitions involved in viral capsid assembly, revealing novel instability and stability conditions for icosahedral states.

## Contribution

It introduces a new theoretical framework that challenges traditional Landau theory by including mixed spherical harmonics and chiral effects in viral capsid assembly.

## Key findings

- Identifies two types of icosahedral solidification transitions.
- Shows stability of odd l icosahedral states requires admixture with neighboring l.
- Highlights the role of chiral terms in lifting degeneracy and affecting transition pathways.

## Abstract

We present a generalized Landau-Brazovskii free energy for the solidification of chiral molecules on a spherical surface in the context of the assembly of viral shells. We encounter two types of icosahedral solidification transitions. The first type is a conventional first-order phase transition from the uniform to the icosahedral state. It can be described by a single icosahedral spherical harmonic of even $l$. The chiral pseudo-scalar term in the free energy creates secondary terms with chiral character but it does not affect the thermodynamics of the transition. The second type, associated with icosahedral spherical harmonics with odd $l$, is anomalous. Pure odd $l$ icosahedral states are unstable but stability is recovered if admixture with the neighboring $l+1$ icosahedral spherical harmonic is included, generated by the non-linear terms. This is in conflict with the principle of Landau theory that symmetry-breaking transitions are characterized by only a \textit{single} irreducible representation of the symmetry group of the uniform phase and we argue that this principle should be removed from Landau theory. The chiral term now directly affects the transition because it lifts the degeneracy between two isomeric mixed-$l$ icosahedral states. A direct transition is possible only over a limited range of parameters. Outside this range, non-icosahedral states intervene. For the important case of capsid assembly dominated by $l=15$, the intervening states are found to be based on octahedral symmetry.