2011
DOI: 10.1103/physrevb.83.165120
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Poynting vector in negative-index metamaterials

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Cited by 42 publications
(63 citation statements)
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“…It is interesting to note that in the presence of loss the contribution of the qT mode to the radiation field does not vanish [the first addend in Eq. (25) does not vanish when p e = p ef ], which is fully consistent with the microscopic theory, because in the case of loss the electric field associated with the qT mode has a small longitudinal component along the z direction.…”
Section: Perfectly Electric Conducting Wiressupporting
confidence: 76%
See 1 more Smart Citation
“…It is interesting to note that in the presence of loss the contribution of the qT mode to the radiation field does not vanish [the first addend in Eq. (25) does not vanish when p e = p ef ], which is fully consistent with the microscopic theory, because in the case of loss the electric field associated with the qT mode has a small longitudinal component along the z direction.…”
Section: Perfectly Electric Conducting Wiressupporting
confidence: 76%
“…Indeed, in general the usual form of the Poynting vector, S = E × H, does not hold in the case of spatially dispersive materials. 24,25 Moreover, there is no known theory to determine the Poynting vector in a general spatially dispersive material, and the only case that is actually understood, and for which closed analytical formulas are available, is when the electromagnetic fields have a spatial variation of the form e −j k·r (plane waves). 24 In this work, we derive closed analytical formulas that enable calculating explicitly the Poynting vector and the electromagnetic energy density in uniaxial wire media for arbitrary electromagnetic field distributions.…”
Section: Introductionmentioning
confidence: 99%
“…Indeed, the importance of the additional term appearing in (36) involving partial derivatives of the constitutive parameters with respect to the wave number to correctly calculate the macroscopic Poynting vector within the framework of an effective medium theory for either natural media or arbitrary metamaterials has been discussed in a few previous works [24,[26][27][28]. Results of numerical comparisons between S av and S h av are presented in the following section dedicated to the homogenization of sample metamaterial structures.…”
Section: E(r)mentioning
confidence: 99%
“…The left-hand side of equation (18) is the stored energy density associated with a natural mode with time dependence e Àixt [39,40,41]. The frequencies x n are the real-valued eigenfrequencies of the natural modes.…”
Section: Overview Of the Eigenfunction Expansion Formalismmentioning
confidence: 99%