Mapping positron annihilation lifetime spectroscopy data of a polymer to classical molecular dynamics simulations without shifting the glass transition temperature

Positron annihilation lifetime spectroscopy (PALS) enables the nondestructive measurement of nanoscale cavities in materials. In this study, a strategy was proposed for mapping PALS measurement data of isotactic polypropylene to classical molecular dynamics (CMD) simulations. The discrepancy between simulated and experimental glass transition temperatures was resolved by shortening the polymer chains, rather than adjusting for the temperature, using the Williams-Landel-Ferry (WLF) equation. The effective probe radii of ortho-positronium (o-Ps), determined by comparing PALS data with CMD simulations, were & SIM;0.8 nm, which was consistent with the o-Ps size given by the solution of the Schrodinger equation. The free-volume fraction corresponding to the effective probe radius was 12.3% at the glass transition temperature, close to the value estimated using Simha-Boyer theory. The cavity number density was proportional to the effective probe radius and decreased with temperature. The o-Ps effective probe radius was proportional to both the critical probe radius and the -1/3 power of the monomer number density, and increased with increasing temperature. These findings suggest that combining PALS measurements with CMD simulations may provide insight into cavities in polymeric materials without relying on the WLF equation.

Automated summary

A strategy was proposed to map PALS measurement data of isotactic polypropylene to CMD simulations, resolving the discrepancy between simulated and experimental glass transition temperatures by shortening polymer chains. The effective probe radius of o-Ps determined by comparing PALS data with CMD simulations was approximately 0.8 nm, consistent with the solution of the Schrodinger equation. Combining PALS measurements with CMD simulations provides insight into cavities in polymeric materials without relying on the WLF equation.