Elasticity theory provides an accurate description of the long-wavelength
vibrational dynamics of homogeneous crystalline solids, and with supplemental
boundary conditions on the displacement field can also be applied to abrupt
heterojunctions and interfaces. The conventional interface boundary conditions,
or connection rules, require that the displacement field and its associated
stress field be continuous through the interface. We argue, however, that these
boundary conditions are generally incorrect for epitaxial interfaces, and we
give the general procedure for deriving the correct conditions, which depend
essentially on the detailed microscopic structure of the interface. As a simple
application of our theory we analyze in detail a one-dimensional model of an
inhomogeneous crystal, a chain of harmonic oscillators with an abrupt change in
mass and spring stiffness parameters. Our results have implications for phonon
dynamics in nanostructures such as superlattices and nanoparticles, as well as
for the thermal boundary resistance at epitaxial interfaces.Comment: 7 pages, Revte