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. 2018 Jul 11;18(8):4927–4933. doi: 10.1021/acs.nanolett.8b01733

Figure 2.

Figure 2

Calculated electric field distribution (YZ planes, for X = 0 μm) from an X-polarized dipole located 5 μm (at Y = −5 μm, Z = 0 μm) from the edge of the plasmonic crystal for three representative wavelengths λ = 1050, 1150, and 1300 nm. The field distribution in the absence of the plasmonic crystal was subtracted for clarity.