Electromagnetic Metasurfaces. Christophe Caloz
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(2.68a)
(2.68b)
which leads, after replacing the instantaneous field vectors by their phaser counterparts, to
(2.69a)
(2.69b)
Third, we write the terms
(2.70a)
(2.70b)
Substituting
(2.71a)
(2.71b)
Finally, rearranging and simplifying the terms in (2.71) leads to