First-principles study on the specific heat jump in the glass transition of silica glass and the Prigogine-Defay ratio

TL;DR

This study uses first-principles molecular dynamics to analyze the glass transition in silica glass, revealing that the specific heat jump is driven by structural energy changes and clarifying the interpretation of the Prigogine-Defay ratio.

Contribution

It introduces a novel analysis of the glass transition using extended state variables and decomposes energy contributions, providing new insights into the Prigogine-Defay ratio in silica glass.

Findings

The specific heat jump is solely due to structural energy changes.

High glass-transition temperature reduces sensitivity of structural energy fluctuations.

The Prigogine-Defay ratio indicates structural energy dominates the transition.

Abstract

The most important characteristic of glass transition is a jump in specific heat $\Delta C_{p}$. Despite its significance, no standard theory exists to describe it. In this study, first-principles molecular-dynamics (MD) simulations are used to describe the glass transition of silica glass, which presents many challenges. The novel view that state variables are extended to include the equilibrium positions of atoms $\{ \bar{\bf R}_{j} \}$ is fully used in analyzing the simulation results. Decomposing the internal energy into three components (structural, phonon, and thermal expansion energies) reveals that the jump $\Delta C_{p}$ of silica glass is entirely determined by the component of structural energy. The reason for the small $\Delta C_{p}$ is its high glass-transition temperature, which makes the fluctuation in the structural energy insensitive to temperature changes. This significantly affects how the Prigogine-Defay ratio $\it{\Pi}$ is interpreted, which was previously unknown. The ratio $\it{\Pi}$ represents the ratio of the total energy change to the contribution of thermal expansion energy at the glass transition. The general property, $\it{\Pi}>1$, of glasses indicates that glass transitions occur mainly by changes in the structural energy. Silica glass is an extreme case in that the transition occurs entirely by the change in internal structure, such as the distribution of the bending angle of Si--O--Si bond.