Abstract:Abstract-The mixed vector and scalar potential formulation is valid from quantum theory to classical electromagnetics. The present rapid development in quantum optics applications calls for electromagnetic solutions that straddle both the quantum and classical physics regimes. The vector potential formulation using A and Φ (or A-Φ formulation) is a good candidate to bridge these two regimes. Hence, there is a need to generalize this formulation to inhomogeneous media. A generalized gauge is suggested for solvi… Show more
“…All these problems can be solved using the decoupled potential formulation (DPIE) presented in [6] . In [7] we find a recent work that goes along similar directions.…”
In this paper we present a numerical implementation of the Decoupled Potential Integral Equation DPIE. The DPIE formulation allows to describe the scattered electromagnetic field by solving a boundary value problem for the vector and scalar potentials A scat and φ scat separately. The formulation allows to obtain the exact scattered electric and magnetic fields for any frequency ω ≥ 0. The formulation is immune to low frequency breakdown, high density mesh breakdown and internal resonances. The formulation can be applied to multiply connected geometries without loop search. In this paper we present a low frequency multilevel fast multipole implementation of the DPIE based on a flat triangular discretization with piecewise constant basis functions and collocation method.
“…All these problems can be solved using the decoupled potential formulation (DPIE) presented in [6] . In [7] we find a recent work that goes along similar directions.…”
In this paper we present a numerical implementation of the Decoupled Potential Integral Equation DPIE. The DPIE formulation allows to describe the scattered electromagnetic field by solving a boundary value problem for the vector and scalar potentials A scat and φ scat separately. The formulation allows to obtain the exact scattered electric and magnetic fields for any frequency ω ≥ 0. The formulation is immune to low frequency breakdown, high density mesh breakdown and internal resonances. The formulation can be applied to multiply connected geometries without loop search. In this paper we present a low frequency multilevel fast multipole implementation of the DPIE based on a flat triangular discretization with piecewise constant basis functions and collocation method.
“…which is the static case of the A-equation in [19], with ε, μ, and α being the permittivity, permeability, and gauge factor, respectively. Meanwhile, the generalized Lorenz gauge…”
Section: A Governing Equationmentioning
confidence: 99%
“…In contrast to the traditional Coulomb gauged method, both the uniqueness and the vectorial nature of A are reserved in this paper. The generalized Coulomb gauge, which is the reduced form of the generalized Lorenz gauge [19] at static limit, is introduced to remove the null space of the curl operator and guarantees the uniqueness of A. To retain the vectorial property of A, it is expanded by the edge elements, and appropriate expansion of the gauge term is formulated based on the space mapping between the Whitney forms by mathematical operators (gradient, divergence, and curl operators) [20], [21], and the Hodge operators [22], [23].…”
In this paper, a solution to the double curl equation with generalized Coulomb gauge is proposed based on the vectorial representation of the magnetic vector potential. Traditional Coulomb gauge is applied to remove the null space of the curl operator and hence the uniqueness of the solution is guaranteed. However, as the divergence operator cannot act on edge elements (curl-conforming) directly, the magnetic vector potential is represented by nodal elements, which is too restrictive, since both the tangential continuity and the normal continuity are required. Inspired by the mapping of Whitney forms by mathematical operators and Hodge (star) operators, the divergence of the magnetic vector potential, as a whole, can be approximated by Whitney elements. Hence, the magnetic vector potential can be expanded by the edge elements, where its vectorial nature is retained and only the tangential continuity is required. Finally, the original equation can be rewritten in a generalized form and solved in a more natural and accurate way using finite-element method.
“…DPIE was implemented numerically by using Nyström method in [23]. A similar idea of exploiting generalized gauge based A-Φ integral formulation was introduced in [24] and its numerical implementation was presented in [25].…”
Abstract-The electric field integral equation is a well known workhorse for obtaining fields scattered by a perfect electric conducting (PEC) object. As a result, the nuances and challenges of solving this equation have been examined for a while. Two recent papers motivate the effort presented in this paper. Unlike traditional work that uses equivalent currents defined on surfaces, recent research proposes a technique that results in well conditioned systems by employing generalized Debye sources (GDS) as unknowns. In a complementary effort, some of us developed a method that exploits the same representation for both the geometry (subdivision surface representations) and functions defined on the geometry, also known as isogeometric analysis (IGA). The challenge in generalizing GDS method to a discretized geometry is the complexity of the intermediate operators. However, thanks to our earlier work on subdivision surfaces, the additional smoothness of geometric representation permits discretizing these intermediate operations. In this paper, we employ both ideas to present a well conditioned GDS-EFIE. Here, the intermediate surface Laplacian is well discretized by using subdivision basis. Likewise, using subdivision basis to represent the sources, results in an efficient and accurate IGA framework. Numerous results are presented to demonstrate the efficacy of the approach.
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