Flexoelectricity from density-functional perturbation theory

We derive the complete flexoelectric tensor, including electronic and lattice-mediated effects, of an arbitrary insulator in terms of the microscopic linear response of the crystal to atomic displacements. The basic ingredient, which can be readily calculated from first principles in the framework of density-functional perturbation theory, is the quantum-mechanical probability current response to a long-wavelength acoustic phonon. Its second-order Taylor expansion in the wave vector $\mathbf{q}$ around the $\Gamma$ ($\mathbf{q}=0$) point in the Brillouin zone naturally yields the flexoelectric tensor. At order one in $\mathbf{q}$ we recover Martin's theory of piezoelectricity [Martin, Phys. Rev. B 5, 1607 (1972)], thus providing an alternative derivation thereof. To put our derivations on firm theoretical grounds, we perform a thorough analysis of the nonanalytic behavior of the dynamical matrix and other response functions in a vicinity of $\Gamma$. Based on this analysis, we find that there is an ambiguity in the specification of the “zero macroscopic field” condition in the flexoelectric case; such arbitrariness can be related to an analytic band-structure term, in close analogy to the theory of deformation potentials. As a by-product, we derive a rigorous generalization of the Cochran-Cowley formula [Cochran and Cowley, J. Phys. Chem. Solids $\mathbf{23}$, 447 (1962)] to higher orders in $\mathbf{q}$. This can be of great utility in building reliable atomistic models of electromechanical phenomena, as well as for improving the accuracy of the calculation of phonon dispersion curves. Finally, we discuss the physical interpretation of the various contributions to the flexoelectric response, either in the static or dynamic regime, and we relate our findings to earlier theoretical works on the subject.

Figure 1

Individual components of the strain gradient tensor in a square two-dimensional lattice. The “longitudinal” (${\varepsilon }_{1,11}$), “shear” (${\varepsilon }_{12,1}$), and “transverse” (or “bending,” ${\varepsilon }_{11,2}$) components are linearly independent; a fourth pattern of less obvious physical interpretation (${\eta }_{1,12}$) is a combination of ${\varepsilon }_{12,1}$ and ${\varepsilon }_{11,2}$. Direction 1 corresponds to the horizontal axis, 2 to the vertical; the polarization vector is oriented along 2.

Figure 2

Displacement fields in longitudinal (top) and transversal (bottom) sound waves.