2012
DOI: 10.1002/mma.2627
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Time domain study of the Drude–Born–Fedorov model for a class of heterogeneous chiral materials

Abstract: Abstract. We deal with the well-posedness of the transient Maxwell equations in a particular class of heterogeneous chiral material modeled by the Drude-Born-Fedorov constitutive relations. A new formulation of the underlying evolution problem allows us to correct a previous result establishing the existence and uniqueness of the electromagnetic fields in a homogeneous medium.1. Introduction. Chiral materials are examples of media which respond with both electric and magnetic polarization to either electric or… Show more

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Cited by 6 publications
(5 citation statements)
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“…In the applied math community, the forward problem for chiral media has excited interest during the past years, see for example [1,2,5,12,13,26,[34][35][36]. In particular, we refer to [37] for recent mathematical developments on chiral media.…”
mentioning
confidence: 99%
“…In the applied math community, the forward problem for chiral media has excited interest during the past years, see for example [1,2,5,12,13,26,[34][35][36]. In particular, we refer to [37] for recent mathematical developments on chiral media.…”
mentioning
confidence: 99%
“…Maxwell's equations supplemented with the previous initial‐boundary conditions, under the non‐autonomous constitutive relations , lead to the following initial‐boundary value problem for E and H : }ϵ∂tMathClass-open(IMathClass-bin+βMathClass-open(tMathClass-close)curlMathClass-close)EMathClass-rel=curlHMathClass-bin−Je1emnbsp1emnbspin1emnbsp1emnbspΩMathClass-punc,1emnbsp1emnbsptMathClass-rel>0MathClass-punc,μ∂tMathClass-open(IMathClass-bin+βMathClass-open(tMathClass-close)curlMathClass-close)HMathClass-rel=MathClass-bin−curlEMathClass-bin−Jm1emnbspin1emnbsp1emnbspΩMathClass-punc,1emnbsp1emnbsptMathClass-rel>0MathClass-punc,divEMathClass-rel=divHMathClass-rel=01emnbsp1emnbspin1emnbsp1emnbspΩMathClass-punc,1emnbsp1emnbsptMathClass-rel≥0MathClass-punc,EMathClass-bin⋅nMathClass-rel=HMathClass-bin⋅nMathClass-rel=curlEMathClass-bin⋅nMathClass-rel=curlHMathClass-bin⋅nMathClass-rel=01emnbsp1emnbsp1emnbsp1emnbspon1emnbsp∂ΩMathClass-punc,1emnbsp1emnbsptMathClass-rel≥0MathClass-punc,EMathClass-open(MathClass-bin⋅MathClass-punc,0MathClass-close)MathClass-rel=E0MathClass-punc,1emnbsp1emnbsp1emnbspHMathClass-open(MathClass-bin⋅MathClass-punc,0MathClass-close)MathClass-rel=H01emnbsp1emnbsp1emnbspin1emnbsp1emnbspfalsemml-overlineΩ¯MathClass-punc. As we can see from the set of equations and the assumptions on the source term, a suitable functional space in which a corresponding Cauchy problem that deals with both E and H can be posed, is the closed space H = W × W , where W = H (div0; Ω) ∩ H 0 (div; Ω) . In fact H , as a closed subspace of L 2 (Ω) 3 × L 2 (Ω) 3 , is also a Hilbert space.…”
Section: Formulation Of the Problemmentioning
confidence: 99%
“…As we can see from the set of equations (3) and the assumptions on the source term, a suitable functional space in which a corresponding Cauchy problem that deals with both E and H can be posed, is the closed space H D W W, where W D H.div0; / \ H 0 .div; / [9,11,12]. In fact H, as a closed subspace of L 2 .…”
Section: The Initial-boundary Value Problemmentioning
confidence: 99%
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“…The topic of electromagnetic propagation and scattering in complex media has recently received an increasing amount of interest from mathematicians. Theoretical analysis for the direct problem in both the time domain and frequency domain can be found in [1,3,4,10,11,31,32,36,37]. We particularly refer to the book [37] for an account of the most recent mathematical results on complex media electromagnetics.…”
Section: Introductionmentioning
confidence: 99%