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Ferroelectricity in dipolar liquids: from an exactly solvable model in the large-dimensional limit to finite dimensions

M. G. Izzo

TL;DR

This work shows that ferroelectric order can emerge in dipolar liquids when the positional degrees of freedom are annealed and the dipolar interaction is regularized to be isotropic and short-ranged. In the $d\to\infty$ limit, a density-functional framework with a second-virial truncation yields an exact result where the excess free energy is minimized by full dipole alignment, despite screening of the long-range tail by orientational averaging. Finite-$d$ extensions use an optimized cluster (renormalized) approach, proving that the second-order virial contribution is still minimized by ferroelectric order for $d\ge3$, with the exponential approximation providing broad validity beyond low densities. Overall, the paper argues that annealed positional disorder is a universal, constitutive driver of ferroelectricity in dipolar liquids, yielding a universal, screened, ferroelectric-like interaction and suggesting avenues to study quenched disorder and dipolar glasses via replicated-liquid theory.

Abstract

A medium, liquid in its positional degrees of freedom, exhibits in real space a homogeneous single-particle density and an isotropic linear response to perturbations of the density field. Under the hypothesis that, if the anisotropic dipolar interaction is a weak perturbation of the isotropic reference system potential, this condition persists in a dipolar liquid for any dipole configuration, a regularization of the dipolar potential can be introduced. This developments lead to the definition of a screened dipolar interaction that is isotropic, short-ranged, and ferroelectric-like. In a classical density functional theory framework the model is exactly solvable in the limit of infinite dimensions, whereas approximations can be obtained in the case of finite dimensions $d \geq 3$ in the optimized cluster expansion scheme. In both cases, it is shown that the system can support a ferroelectric phase transition. The study relates the emergence of ferroelectricity in dipolar liquids to a constitutive property of the liquid state, i.e. annealed positional disorder.

Ferroelectricity in dipolar liquids: from an exactly solvable model in the large-dimensional limit to finite dimensions

TL;DR

This work shows that ferroelectric order can emerge in dipolar liquids when the positional degrees of freedom are annealed and the dipolar interaction is regularized to be isotropic and short-ranged. In the limit, a density-functional framework with a second-virial truncation yields an exact result where the excess free energy is minimized by full dipole alignment, despite screening of the long-range tail by orientational averaging. Finite- extensions use an optimized cluster (renormalized) approach, proving that the second-order virial contribution is still minimized by ferroelectric order for , with the exponential approximation providing broad validity beyond low densities. Overall, the paper argues that annealed positional disorder is a universal, constitutive driver of ferroelectricity in dipolar liquids, yielding a universal, screened, ferroelectric-like interaction and suggesting avenues to study quenched disorder and dipolar glasses via replicated-liquid theory.

Abstract

A medium, liquid in its positional degrees of freedom, exhibits in real space a homogeneous single-particle density and an isotropic linear response to perturbations of the density field. Under the hypothesis that, if the anisotropic dipolar interaction is a weak perturbation of the isotropic reference system potential, this condition persists in a dipolar liquid for any dipole configuration, a regularization of the dipolar potential can be introduced. This developments lead to the definition of a screened dipolar interaction that is isotropic, short-ranged, and ferroelectric-like. In a classical density functional theory framework the model is exactly solvable in the limit of infinite dimensions, whereas approximations can be obtained in the case of finite dimensions in the optimized cluster expansion scheme. In both cases, it is shown that the system can support a ferroelectric phase transition. The study relates the emergence of ferroelectricity in dipolar liquids to a constitutive property of the liquid state, i.e. annealed positional disorder.

Paper Structure

This paper contains 6 sections, 58 equations.