Generic role of the anisotropic surface free energy on the morphological evolution in a strained-heteroepitaxial solid droplet on a rigid substrate

TL;DR

This study uses self-consistent dynamical simulations to explore how anisotropic surface free energy influences the morphological evolution of strained heteroepitaxial solid droplets, revealing distinct stability and growth modes.

Contribution

It provides a detailed analysis of the effects of surface energy anisotropy and symmetry on droplet morphology and evolution in heteroepitaxial systems, highlighting new morphological modes.

Findings

Formation of a thin wetting layer during island development

Existence of stable Cosine-shaped droplets above a threshold anisotropy

Identification of Frank-van der Merwe thin film mode at high anisotropy

Abstract

A systematic study based on the self-consistent dynamical simulations is presented for the spontaneous evolution of an isolated thin solid droplet on a rigid substrate, which is driven by the surface drift diffusion induced by the anisotropic capillary forces (surface stiffness) and mismatch stresses. In this work, we studied the affect of surface free energy anisotropies on the development kinetics of the 'Stranski-Krastanow' island type morphology. The anisotropic surface free energy and the surface stiffness were treated with well accepted trigonometric functions. Although, various tilt angles and anisotropy constants were considered during simulations, the main emphasis was given on the effect of rotational symmetries associated with the surface Helmholtz free energy topography in 2D space. Our computer simulations revealed the formation of an extremely thin wetting layer during the development of the bell-shaped Stranski-Krastanow island through the mass accumulation at the central region of the droplet via surface drift-diffusion. In the strong (anomalous) anisotropy constant domain, we demonstrated the existence of two distinct morphological modes: i) the complete stability of the initial Cosine-shaped droplet just above a certain anisotropy constant threshold level by spontaneous slight readjustments of the base and the height of the cluster; ii) the Frank-van der Merwe mode of thin film formation for very large values of the anisotropy constant by the spreading and coalescence of the droplets over the substrate surface. During the course of the simulations, we have continuously tracked both the morphology (i.e., the peak height, the extension of the wetting layer beyond the domain boundaries, and the triple junction contact angle) and energetic (the global Helmholtz free energy changes associated with the total strain and surface energy variations) of the system.