Browsing by Author "Beale, J Thomas"
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Item Open Access A Third Order Numerical Method for Doubly Periodic Electromegnetic Scattering(2007-07-31) Nicholas, Michael JWe here developed a third-order accurate numerical method for scattering of 3D electromagnetic waves by doubly periodic structures. The method is an intuitively simple numerical scheme based on a boundary integral formulation. It involves smoothing the singular Green's functions in the integrands and finding correction terms to the resulting smooth integrals. The analytical method is based on the singular integral methods of J. Thomas Beale, while the scattering problem is motivated by the 2D work of Stephanos Venakides, Mansoor Haider, and Stephen Shipman. The 3D problem was done with boundary element methods by Andrew Barnes. We present a method that is both more straightforward and more accurate. In solving these problems, we have used the M\"{u}ller integral equation formulation of Maxwell's equations, since it is a Fredholm integral equation of the second kind and is well-posed. M\"{u}ller derived his equations for the case of a compact scatterer. We outline the derivation and adapt it to a periodic scatterer. The periodic Green's functions found in the integral equation contain singularities which make it difficult to evaluate them numerically with accuracy. These functions are also very time consuming to evaluate numerically. We use Ewald splitting to represent these functions in a way that can be computed rapidly.We present a method of smoothing the singularity of the Green's function while maintaining its periodicity. We do local analysis of the singularity in order to identify and eliminate the largest sources of error introduced by this smoothing. We prove that with our derived correction terms, we can replace the singular integrals with smooth integrals and only introduce a error that is third order in the grid spacing size. The derivation of the correction terms involves transforming to principal directions using concepts from differential geometry. The correction terms are necessarily invariant under this transformation and depend on geometric properties of the scatterer such as the mean curvature and the differential of the Gauss map. Able to evaluate the integrals to a higher order, we implement a \mbox{GMRES} algorithm to approximate solutions of the integral equation. From these solutions, M\"{u}ller's equations allow us to compute the scattered fields and transmission coefficients. We have also developed acceleration techniques that allow for more efficient computation.We provide results for various scatterers, including a test case for which exact solutions are known. The implemented method does indeed converge with third order accuracy. We present results for which the method successfully resolves Wood's anomaly resonances in transmission.Item Open Access Maximum Norm Regularity of Implicit Difference Methods for Parabolic Equations(2011) Pruitt, MichaelWe prove maximum norm regularity properties of L-stable finite difference
methods for linear-second order parabolic equations with coefficients
independent of time, valid for large time steps. These results are almost
sharp; the regularity property for first differences of the numerical solution
is of the same form as that of the continuous problem, and the regularity
property for second differences is the same as the continuous problem except for
logarithmic factors.
This generalizes a result proved by Beale valid for the constant-coefficient
diffusion equation, and is in the spirit of work by Aronson, Widlund and
Thomeé.
To prove maximum norm regularity properties for the homogeneous problem,
we introduce a semi-discrete problem (discrete in space, continuous in time).
We estimate the semi-discrete evolution operator and its spatial differences on
a sector of the complex plan by constructing a fundamental solution.
The semi-discrete fundamental solution is obtained from the fundamental solution to the frozen coefficient problem by adding a correction term found through an iterative process.
From the bounds obtained on the evolution operator and its spatial differences,
we find bounds
on the resolvent of the discrete elliptic operator and its differences through
the Laplace transform
representation of the resolvent. Using the resolvent estimates and the
assumed stability properties of the time-stepping method in the Cauchy integral
representation of the fully discrete solution operator
yields the homogeneous regularity result.
Maximum norm regularity results for the inhomogeneous
problem follow from the homogeneous results using Duhamel's principle. The results for the inhomogeneous
problem
imply that when the time step is taken proportional to the grid width, the rate of convergence of the numerical solution and its first
differences is second-order in space, and the rate of convergence for second
differences
is second-order except for logarithmic factors .
As an application of the theory, we prove almost sharp maximum norm resolvent estimates for divergence
form elliptic operators on spatially periodic grid functions. Such operators are invertible, with inverses and their first differences bounded in maximum norm, uniformly in the grid width. Second differences of the inverse operator are bounded except for logarithmic factors.
Item Open Access On Computing Smooth, Singular, and Nearly Singular Integrals on Implicitly Defined Surfaces(2010) Wilson, Jason R.We present numerical methods for the approximation of smooth, singular, and nearly singular integrals on implicitly defined surfaces. We begin with a high-order quadrature formula for an integral over a compact smooth implicitly defined hypersurface. Our high-order formula is novel in that it has spectral convergence but does not require a set of overlapping patches. Rather, certain hypersurface points, called quadrature points, must be determined. To find the quadrature points, we search for certain line segments, called brackets, for which the level set function has a sign change at the endpoints. We show that as the segment spacing tends to zero, that each quadrature point must be eventually contained in exactly one bracket. To find the quadrature point within a bracket we use standard one dimensional root finding techniques. Next, we show how to accelerate the process of finding the brackets by restricting the line segment search to cells that are near the hypersurface. Finally, we give an optimal algorithm for finding the quadrature points that has an observed runtime proportional to the number of quadrature points. The high-order convergence of our new quadrature formula is demonstrated numerically on a number of complex implicitly defined surfaces and smooth integrands. Using standard interpolation and finite differencing techniques, we show how to achieve high-order accuracy in the case where the level-set function and integrand are only known at regularly spaced grid points.
We next address the problem of computing double layer and single layer potentials. By using a locally flat cutoff function, we decompose the layer potential into a global part and a local part. We numerically verify that our new quadrature formula has high-order convergence when applied to the global part of a singular double layer potential by computing Gauss's integral on a number of complex implicitly defined surfaces. For the local part, we focus on the single layer potential. In particular, we give a constant runtime complexity algorithm for evaluating the local part of a single layer potential for both the singular and nearly singular cases. To compute the local part, we write the integral in certain local polar coordinates and consider the angular and radial parts separately. We first prove that the angular part can be approximated to high order using the trapezoid rule. In particular, we show that due to our choice of local coordinates, the integrand of the angular part is well approximated by a low degree trigonometric polynomial which is integrated exactly by the trapezoid rule with a small number of quadrature points. We next show that by multiplying the radial integrands by certain helper functions and using a change of variable, the radial integrals can be written in terms of standard integrals that can be precomputed and stored in a lookup table. We demonstrate the high-order convergence of our constant runtime local single layer potential integration method with a number of numerical examples on complex implicitly defined surfaces.