SearcharxivSearch

arXiv subjects

Gerald D. Mahan

Publications and source records attributed to Gerald D. Mahan.

3 recordsLinked to original sources

Theory of Electron-Phonon-Dislon Interacting System - Toward a Quantized Theory of Dislocations

We provide a comprehensive theoretical framework to study how crystal dislocations influence the functional properties of materials, based on the idea of quantized dislocation, namely a "dislon". In contrast to previous work on dislons which focused on exotic phenomenology, here we focus on the theoretical structure and computational power. We first provide a pedagogical introduction of the necessity and benefits taking the dislon approach, that why the dislon Hamiltonian takes its current form. Then we study the electron-dislocation and phonon-dislocation scattering problems, using the dislon formalism. Both the effective electron and phonon theories are derived, from which the role of dislocations on electronic and phononic transport properties is computed. Comparing with the traditional dislocation scattering studies which are intrinsically single-particle, low-order perturbation and classical quenched defect in nature, the dislon theory not only allows easy incorporation of quantum many-body effects such as electron correlation, electron-phonon interaction and higher-order scattering events, but also allows proper consideration of dislocation's long-range strain field and the dynamic aspects on equal footing. This means that instead of developing individual model for a specific dislocation scattering problem, the dislon theory allows for the calculation of electronic structure and electrical transport, thermal transport, optical and superconducting properties, etc., under one unified theory. Furthermore, the dislon theory has another advantage over empirical models in that it requires no fitting parameters. The dislon theory could serve as a major computational tool to understand the role of dislocations on multiple materials' functional properties at an unprecedented level of clarity, and may have wide applications in dislocated energy materials.

cond-mat.mtrl-sci

Lattice dynamics model calculation of Kapitza conductance at solid-fluid interfaces

Existing theoretical models of the interfacial thermal conductance, i.e., Kapitza conductance, of insulating solid-fluid interfaces only consider bulk properties, e.g., acoustic mismatch model and diffuse mismatch model. In this work, we propose a classical lattice dynamical model calculation of the Kapitza conductance, thereby incorporating interfacial structural details. In our model, we assume that heat is mostly carried by phonons in the solid, and that sound waves carry diffusive heat from the interface into the bulk of the liquid, where both longitudinal and transverse sound waves are considered. Sound wave dispersion is calculated from the fluid pair distribution function, evaluated using approximate integral equation theories (i.e., Percus-Yevick, Hypernetted-chain approximation). The Kapitza conductance of the solid-fluid interface is obtained from the phonon transmission coefficient at the interface. We determine the interfacial phonon transmission coefficient by solving the coupled equations of motion for the interfacial solid and fluid atoms. As an illustrative example, we derive the Kapitza conductance of solid argon-fluid neon interface, with pair-wise Lennard-Jones interactions.

cond-mat.mtrl-sci

Pair Distribution Function of a Square-Well Fluid

The properties of the ground state of liquid $^4$He are studied using a correlated basis function of the form $\prod_{i<j} ψ(r_{ij})$. Here, $ψ(r)$ is chosen as the exact solution of the Schrödinger equation for two $^4$He atoms. A hard-sphere plus an attractive square well is used as the interaction potential between $^4$He atoms. The pair distribution function is calculated using approximate integral methods, namely the Percus-Yevick (PY) equation and Hypernetted Chain (HNC) approximation. The values thus obtained are used to calculate the ground state energy, which is found to be -4.886 K using the PY equation. The liquid structure factor is also obtained using the pair distribution function. The values for the pair distribution function and liquid structure factor are compared with experimental results and earlier theoretical calculations.

cond-mat.other