By Mackay, Tom G.; Lakhtakia, Akhlesh
The themes of anisotropy and bianisotropy are basic to electromagnetics from either theoretical and experimental views. those homes underpin a number of complicated and unique electromagnetic phenomenons in certainly taking place fabrics and in relativistic eventualities, in addition to in artificially produced metamaterials. As a special consultant to this speedily constructing box, this publication presents scholars and execs with a unified presentation of key vintage and up to date effects at the stories of constitutive kin, spacetime symmetries, planewave propagation, dyadic eco-friendly capabilities, and homogenization of composite fabrics. This booklet additionally deals an updated extension to straightforward remedies of crystal optics with insurance on either linear and weakly nonlinear regimes.
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Additional info for Electromagnetic Anisotropy and Bianisotropy - A Field Guide
6) A key property of isotropic chiral mediums is that they exhibit optical activity . That is, they can distinguish between left–handed and right–handed electromagnetic ﬁelds. Measures of optical activity due to an isotropic chiral medium and its mirror conjugate diﬀer only in sign. 3). Since an isotropic chiral medium exhibits the same measures of optical activity in all directions, its optical activity is often designated as natural optical activity. Notice that, in view of the deﬁnition presented in Sec.
26] L. Onsager, Reciprocal relations in irreversible processes. I, Phys Rev 37 (1931), 405–426.  L. Onsager, Reciprocal relations in irreversible processes. II, Phys Rev 38 (1931), 2265–2279. G. Casimir, On Onsager’s principle of microscopic reversibility, Rev Mod Phys 17 (1945), 343–350. B. F. Greene, On a theorem of irreversible thermodynamics, Phys Rev 86 (1952), 702–710. B. L. L. Jackson, Statistical mechanics of irreversibility, Phys Rev 88 (1952), 1382–1386.  A. A. Depine, On Onsager relations and linear electromag¨ 59 (2005), 101–104.
17) By virtue of the principle of causality, the imaginary parts of the ω– dependent permittivity scalars x , y and z are positive–valued for a dissipative medium. 17) can be mathematically convenient, but are not particularly insightful. 18) 36 Electromagnetic Anisotropy and Bianisotropy: A Field Guide highlights the biaxial symmetry via the two unit vectors u ˆ m and u ˆn . In the absence of dissipation, the ω–dependent permittivity scalars p and ˆm and u ˆn are aligned with the q are real–valued and the unit vectors u optic ray axes.
Electromagnetic Anisotropy and Bianisotropy - A Field Guide by Mackay, Tom G.; Lakhtakia, Akhlesh