1999
DOI: 10.1103/physrevb.60.6459
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Lattice dynamics of a disordered solid-solid interface

Abstract: Generic properties of elastic phonon transport at a disordered interface are studied. The results show that phonon transmittance is a strong function of frequency and the disorder correlation length. At frequencies lower than the van Hove singularity the transmittance at a given frequency increases as the correlation length decreases. At low frequencies, this is reflected by different power-laws for phonon conductance across correlated and uncorrelated disordered interfaces which are in approximate agreement w… Show more

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Cited by 50 publications
(36 citation statements)
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“…We therefore expect that our conclusions regarding the inelastic effects remain valid also for more complicated pair potentials. The face-centered-cubic lattice has been used as the lattice model in numerous earlier works investigating the effects of various material parameters on interfacial transport, including lattice constant [26] and mass [27] mismatch, the strength of interfacial bonding [10], low-dimensional contacts [28], interface roughness [29][30][31][32], and phonon-mediating thin films [33].…”
Section: A Structurementioning
confidence: 99%
“…We therefore expect that our conclusions regarding the inelastic effects remain valid also for more complicated pair potentials. The face-centered-cubic lattice has been used as the lattice model in numerous earlier works investigating the effects of various material parameters on interfacial transport, including lattice constant [26] and mass [27] mismatch, the strength of interfacial bonding [10], low-dimensional contacts [28], interface roughness [29][30][31][32], and phonon-mediating thin films [33].…”
Section: A Structurementioning
confidence: 99%
“…This approach is not valid for lower energy subgap phonons as their loss rate may be very slow and the temporal response may become dispersive. 13,27,28 In addition, their significant accumulation changes the rates of detrapping through the term I detrap ͕f trap ͖. However, for the moment, we will ignore this group of phonons but will discuss their possible role in the later consideration of real structures and experimental situations.…”
Section: Kinetic Description Of Nonequilibrium Quasiparticles Andmentioning
confidence: 99%
“…For the numerical calculation of the central quantity, T (E), we use a general scattering technique which has been recently formulated for studies of the giant magnetoresistance [20]. Application of the method to phonon transport across disordered interfaces [21] and to electric conductance in multi-wall carbon nanotubes [20] reveals an efficient algorithm for calculating the Green function for arbitrary tight-binding Hamiltonians and, hence, the S-matrix [19]. The computational scheme comprises two essential steps: first, the calculation of an effective (renormalized) interaction between the electrodes by projecting out the degrees of freedom of the scatterer, and second, the computation of the unperturbed electrodes Green function.…”
Section: ) Readsmentioning
confidence: 99%