..
..

The 2007 John H. Barrett Memorial Lectures
..
Multi-Scale Modeling and Simula
tion
in Materials Science

..
April 28th - April 30th
University of Tennessee University of Tennessee, Knoxville
..
...

Schedule/Slides     Accommodations     Map     UTK     UTK Math     ORNL     Home
Russel Caflisch
Univ of California, LA
Growth, Structure and Pattern Formation for Thin Films

An epitaxial thin film consists of layers of atoms whose lattice properties are determined by those of the underlying substrate. This talk will describe mathematical modeling, analysis and simulation of growth, structure and pattern formation for epitaxial systems.

Epitaxial growth involves physics on both atomistic and continuum length scales. For example, diffusion of adatoms can be coarse-grained, but nucleation of new islands and breakup for existing islands are best described atomistically. Our growth simulations use an island dynamics model with a level set simulation method. The level set velocity comes from a detailed model for a step edge or island boundary on an epitaxial surface. Through asymptotic analysis of this model, we derive the Gibbs-Thomson formula for anisotropic step stiffness.

In heteroepitaxial growth, e.g., Germanium on Silicon, mismatch between the lattice spacing of the Silicon substrate and the Germanium film will introduce a strain into the film, which can significantly influence the material structure, for example leading to formation of quantum dots. Strain computations can be computationally intensive, so that effective simulation of atomistic strain effects relies on an accelerated method that incorporates algebraic multigrid and an artificial boundary condition.

Technological applications of epitaxial structures, such as quantum dot arrays, require a degree of geometric uniformity that has been difficult to achieve. Modeling and simulation may contribute insights that will help to overcome this problem. We present simulations that combine growth and strain showing spontaneous and directed self-assembly of patterns in epitaxial systems. These include alloy segregation, laterally aligned islands and wires, and vertically aligned quantum dots.
Bjorn Engquist
Univ of Texas, Austin
Heterogeneous Multi-Scale Methods

Continuum simulations of solids or fluids for which some atomistic information is needed are typical example of multi-scale problems with very large ranges of scales. For such problems it is necessary to restrict the simulations on the micro-scale to a smaller subset of the full computational domain. The heterogeneous multi-scale method is a framework for developing and analyzing numerical methods that couple computations from very different scales. Local micro-scale simulations on small domains supply missing data to a macro-scale simulation on the full domain. Examples are local molecular dynamics computations that produce data to a continuum macro-scale model, or a highly oscillatory dynamical system for which a local estimate of resonances is enough to supply data for a smoother evolution of averages.

In the lectures we will first study the challenge of multi-scale
simulation in general and discuss different classes of potential
strategies. Then the heterogeneous multi-scale method will be introduced together with mathematical analysis and applications
.
Mitchell Luskin
University of Minnesota
Mathematical Results and Challenges for the Quasi Continuum Approximation

In the first lecture, We will derive and compare several quasicontinuum approximations. We will examine the nature of the interactions between the representative atoms near the atomistic interface and compare force-based and energy-based approximations. We will give an analysis proving that the equilibrium equations have a unique solution under suitable restrictions on the loads (less than the limit load), and we will give a convergence rate for an iterative method to solve the equilibrium equations.

The quasicontinuum methodology involves the application of the Cauchy-Born rule to the underlying lattice in continuum regions. The validity of this approximation is dependent on the utilization of a unit cell that does not restrict possible lattice instabilities. At the same time, the computational efficiency of the method relies on the use of a minimal cell size. In the second lecture, We will describe recent work on the development and analysis of an adaptive algorithm to change the element cell size as the element strain evolves during a quasi-static process.

In the third lecture, we will develop an a posteriori error estimator which quantifies the modeling error for a goal function and allows for an adaptive decision about which regions should be modeled as a continuum and which regions should be modeled atomistically. We employ the framework of duality based error estimators to measure the  approximation error to be minimized in terms of a user-definable goal function.

Joint work with Marcel Arndt, Matthew Dobson, Ryan Elliott, and Ellad Tadmor

Gregory Beylkin
Univ of Colorado, Boulder
Fast Algorithms for Adaptive Application of Integral Operators in High Dimensions

In physics, chemistry and other applied fields, many important problems may be formulated using integral equations, typically involving Green's functions as their kernels. Often such formulations are preferable to those via partial differential equations (PDEs). For example, evaluating the integral expressing solution of the Poisson equation in free space, i.e., the convolution of the Green's function with the mass or charge density, avoids issues associated with the high condition number of a PDE formulation. Since many physically significant operators depend only on the distance between interacting objects, the operators such as $(-\Delta+\mu^{2}I)^{-\alpha}$, where $\mu\geq 0$ and $0 <\alpha< 3/2$, and certain singular operators, such as the projector on divergence-free functions, fall into the class of operators for which our approach yields fast adaptive algorithms.

This talk will describe adaptive multi resolution algorithms for applying integral operators with radially symmetric kernels in dimensions one, two and three. In dimensions two and higher kernels of operators are represented in separated form by approximating radial kernels by a sum of Gaussians, for any finite but arbitrary accuracy. We will briefly discuss an extension to dimensions higher than three.

Peter Cummings Vanderbilt and ORNL

Many-Scale and Multi-Scale Modeling in Computational Nanoscience

Theory, modeling and simulation (TMS) tools constitute key enabling technologies for making fundamental advances in nanoscience and for making nanotechnology a practical reality. Many of the problems encountered in this field are inherently multiscale modeling. In this talk, we provide an overview of the role of TMS in nanoscience, as well as an overview of our multiscale TMS research in nanotribology, molecular electronics, and hybrid organic-inorganic nanocomposites.
Qiang Du
Penn State
Quantized Vortices in Superconductors and Bose-Einstein Condensates

Superconductivity is one of the grand challenges identified as being crucial to future economic prosperity and scientific leadership. In
recent years, the analysis and simulations of various mathematical models in superconductivity have attracted the interests of many mathematicians all over the world. Their works have helped us to understand the intriguing and complex phenomena in superconductivity.

A particular focus of the mathematical study of superconductivity is the phenomena of quantized vortices, which is a well-known signature of superfluidity. With the recent award of the Nobel prize in physics to Ginzburg, Abrikosov and Leggett, the spotlight has again been shed on the popular Ginzburg-Landau theory that was proclaimed as "being of great importance in physics ...". There are new and unresolved mathematical challenges be explored further. In this talk, we will briefly review the physical background and discuss some of the analytical and computational issues. Connections to other relevant problems such as the quantized vortices in Bose-Einstein condensates will also be discussed.

George Karniadakis Brown University
A Seamless Multiscale Approach for Modeling Complex Fluids

We will present a stochastic molecular dynamics method, termed Dissipative Particle Dynamics, or DPD, which can bridge the gap between atomistic scales and continuum. In particular, it represents the thermal fluctuations accurately but it is also valid for finite and even high Reynolds number flows. The problems that we address involve both soft and hard potentials and we will present a family of efficient time integration schemes to deal with the multi rate dynamics.
Markos Katsoulakis
Univ of Massachusetts, Amherst
Mathematical Strategies and Error Quantification in the Coarse-Graining of Many-Body Stochastic Systems

In this talk we discuss recent and on going work in obtaining
coarse-grained stochastic approximations of extended (many-body) microscopic systems. Examples of such models will include stochastic lattice dynamics, as well as more complex off-lattice models of macromolecules (e.g. polymers) that have internal degrees of freedom.

Computational comparisons of coarse-grained and microscopic simulations along with accompanying rigorous estimates on the loss of information between the coarse-grained and microscopic probability distribution functions (pdf) highlight the validity regimes and the limitations of the methods. Furthermore we develop spatial adaptivity methods for microscopic simulations, where the adaptivity criterion is based on a posteriori estimates on the loss of information between the coarse-grained and the microscopic pdf. Finally, we demonstrate how statistical mechanics, cluster expansion methods can give rise to improved coarse-graining schemes and effectively compress long-range interactions in stochastic many-body systems.

Leonard Sander University of Michigan
Kinetic Monte Carlo Simulation of Strained Heteroepitaxy in Three Dimensions

Morphological evolution of strained heteroepitaxial films is studied
using a kinetic Monte Carlo method in three dimensions. We generalize a Green's function approach by Lam, Lee, and Sander [Phys. Rev Rev. Lett. 89 89, 216102-1 (2002)]. Isolated islands are observed under deposition conditions for deposition rates slow compared with intrinsic surface roughening rates. They are semi-spherical and truncated conical for high and low temperature cases respectively. Annealing of films at high temperature leads to the formation of closely packed islands consistent with an instability theory. At low temperature, pits form via a layer-by-layer nucleation mechanism and subsequently develop into grooves.
(With C-H Lam and M. T. Lung)
Art Voter
Los Alamos National Laboratory
Accelerated Molecular Dynamics Methods

A significant problem in the atomistic simulation of materials is that molecular dynamics simulations are limited to nanoseconds, while important reactions and diffusive events often occur on time scales of microseconds and longer. Although rate constants for slow events can be computed directly using transition state theory (with dynamical corrections, if desired, to give exact rates), this requires first knowing the transition state. Often, however, we cannot even guess what events will occur. For example, in vapor-deposited metallic surface growth, surprisingly complicated exchange events are pervasive.

I will discuss recently developed methods (hyperdynamics, parallel replica dynamics, and temperature accelerated dynamics) for treating this problem of complex, infrequent-event processes. The idea is to directly accelerate the dynamics to achieve longer times without prior knowledge of the available reaction paths. I will present some recent applications, including metallic surface growth, deformation and dynamics of carbon nanotubes, and annealing after radiation damage events in MgO, and discuss future challenges in the development of these methods.
..
...
Univ of Tennessee
Ayres Hall, UTK
Smoky Mountains
Smoky Mountains
Knoxville, TN
Knoxville