Role of ionic quantum-anharmonic fluctuations on the bond length alternation and giant piezoelectricity of conjugated polymers

TL;DR

This study investigates how ionic quantum-anharmonic fluctuations influence the structural and piezoelectric properties of conjugated polymers, revealing that fluctuations significantly shift phase boundaries but preserve and even enhance giant piezoelectric responses.

Contribution

The paper introduces a stochastic self-consistent harmonic approximation to quantify quantum ionic effects on conjugated polymers, validated against first-principles calculations, and demonstrates their impact on phase transition boundaries and piezoelectricity.

Findings

Quantum fluctuations shift the dimerization phase boundary by 34%.

Giant piezoelectricity persists despite large bond length fluctuations.

Quantum effects enhance effective charges and optimize piezoelectric response.

Abstract

Functionalized conjugated polymers are promising materials for electromechanical applications due to predicted giant piezoelectricity, arising from anomalously large dynamical effective charges and an enhanced response in the proximity of the dimerization phase transition. In this work, we assess the impact of quantum ionic fluctuations on piezoelectricity using the stochastic self-consistent harmonic approximation with a Rice-Mele diatomic chain model, parametrized to reproduce hybrid-functional first-principles calculations of prototypical carbyne. The model's accuracy is validated against first-principles calculations both with and without quantum-anharmonic effects. We find that ionic fluctuations strongly impact the structural properties, with the boundary of the dimerization phase transition shifted by $34\%$. Despite quantum fluctuations in the bond length reaching magnitudes comparable to the average, the strong piezoelectric response persists. The topological enhancement of the effective charges remains robust and is even enhanced by about $\sim20\%$ thanks to a quantum-induced shrinking of the electronic gap. The piezoelectric coefficient remains dominated by the internal relaxation and retains a morphotropic-like character, reaching maximum values near the renormalized boundary, with quantum anharmonicity mainly shifting the optimal enhancement window.