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Because of the strong dual asymmetry, the fields are often described by the electric characteristics only (e.g., (Equation presented), etc.), but these are not fundamental characteristics of free Maxwell fields [3,12,13].
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The "magnetoelectric energy density" can also be thought of as proportional to the "imaginary helicity" (Equation presented), while the "magnetoelectric momentum density" (20) and "magnetoelectric spin density" (21) involve the "imaginary Poynting vector" (Equation presented). The latter is known as an alternating flow of stored energy [, 3rd ed. (Wiley, New York).].
-
The "magnetoelectric energy density" can also be thought of as proportional to the "imaginary helicity" (Equation presented), while the "magnetoelectric momentum density" (20) and "magnetoelectric spin density" (21) involve the "imaginary Poynting vector" (Equation presented). The latter is known as an alternating flow of stored energy [J.D. Jackson, Classical Electrodynamics, 3rd ed. (Wiley, New York, 1999).].
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Note that the resonant magnetoelectric response, Eq. (25) and Fig. 1, cannot be mixed up with the resonant chiral response in [6,9] because the latter vanishes for equal amplitudes of the counterpropagating waves and also has a symmetric rather than antisymmetric profile in the vicinity of the nodal points [Fig. 1(b)].
-
Note that the resonant magnetoelectric response, Eq. (25) and Fig. 1, cannot be mixed up with the resonant chiral response in [6,9] because the latter vanishes for equal amplitudes of the counterpropagating waves and also has a symmetric rather than antisymmetric profile in the vicinity of the nodal points [Fig. 1(b)].
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