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. 2015 Apr 9;5(2):577–613. doi: 10.3390/nano5020577

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© 2015 by the authors; licensee MDPI, Basel, Switzerland

This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution license (http://creativecommons.org/licenses/by/3.0/).

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Figure 1. — (a) Faraday rotation by a magneto-plasmonic photonic crystal for the TM-polarised incident light, where φ is the Faraday rotation angle. At normal incidence, TM-polarised light has the electric field perpendicular to the gold wires; (b) Schematic of the magneto-optical photonic crystal, where the BIG film (dark red) is deposited on a glass substrate (blue) and the periodic gold nanowire structure is sitting atop; (c) A scanning electron microscopy image of one of the investigated hybrid structures; (d) Measured Faraday rotation of the three samples at normal incidence (TM polarization), compared with measured Faraday rotation of the bare BIG film; (e) Measured transmittance of the three samples at normal incidence (TM polarization). Reprinted from [44] with permission by Macmillan Publishers Ltd, Copyright 2013.

Figure 1. — (a) Faraday rotation by a magneto-plasmonic photonic crystal for the TM-polarised incident light, where φ is the Faraday rotation angle. At normal incidence, TM-polarised light has the electric field perpendicular to the gold wires; (b) Schematic of the magneto-optical photonic crystal, where the BIG film (dark red) is deposited on a glass substrate (blue) and the periodic gold nanowire structure is sitting atop; (c) A scanning electron microscopy image of one of the investigated hybrid structures; (d) Measured Faraday rotation of the three samples at normal incidence (TM polarization), compared with measured Faraday rotation of the bare BIG film; (e) Measured transmittance of the three samples at normal incidence (TM polarization). Reprinted from [44] with permission by Macmillan Publishers Ltd, Copyright 2013.