2014
DOI: 10.2528/pier14052608
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Mixed Finite Element Method for 2d Vector Maxwell's Eigenvalue Problem in Anisotropic Media

Abstract: Abstract-It is well known that the conventional edge element method in solving vector Maxwell's eigenvalue problem will lead to the presence of nonphysical zero eigenvalues. This paper uses the mixed finite element method to suppress the presence of these nonphysical zero eigenvalues for 2D vector Maxwell's eigenvalue problem in anisotropic media. We introduce a Lagrangian multiplier to deal with the constraint of divergence-free condition. Our method is based on employing the first-order edge element basis fu… Show more

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Cited by 18 publications
(9 citation statements)
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“…As it is usual for treating equality constraints (see [19,20,21]), we are going to introduce a Lagrange multiplier in the space ker T . This leads us to write the following mixed problem…”
Section: A First Stabilized Mixed Formulationmentioning
confidence: 99%
See 1 more Smart Citation
“…As it is usual for treating equality constraints (see [19,20,21]), we are going to introduce a Lagrange multiplier in the space ker T . This leads us to write the following mixed problem…”
Section: A First Stabilized Mixed Formulationmentioning
confidence: 99%
“…The last two equations of (146) show that it is equivalent to say that the solution ϕ h belongs to a subspace of V h of co-dimension dim M h + 3. This subspace is not a subspace of V N , in other words we realize a non-conform approximation of the space V N and that is why the multiplier η h is not 0 (see remark 9.1 in [20] and [21] for similar situations).…”
mentioning
confidence: 99%
“…. The transverse components of electromagnetic field are directly obtained from the equations ( 10)- (11). This is so called TEM mode.…”
Section: Governing Equations For Waveguide Problemsmentioning
confidence: 99%
“…t e t ) = 0. But we can not omit the divergence-free condition ∇ t • (µ −1 t e t ) = 0 in numerical computation, otherwise PDEs (25) will introduce spurious zero modes [11]. Because ∇ t • (µ −1 t e t ) = 0 and (18), we can get 1 µ+ab ∇ t • ( t e t ) = 0, then ∇ t • ( t e t ) = 0, which is just Gauss' law for electric field.…”
Section: A Simulate Te Modes Using Longitudinalmentioning
confidence: 99%
“…In this paper, we develop an efficient numerical algorithm for solving the Maxwell eigenvalue problem which plays an important role in computational electromagnetism (see, e.g., [3,4,12,15,16,18]). The governing equations are…”
Section: Introductionmentioning
confidence: 99%