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. 2016 Feb;472(2186):20150658. doi: 10.1098/rspa.2015.0658

Figure 14.

Figure 14.

(a) Isofrequency curves for the second surface for a rectangular lattice with dx=1, dy=2. The angle of incidence ψ=π/4, the dashed line κy=3.1113 and the ambient medium's contour β2=4.42=κx2+κy2 are also shown. The predicted directions of propagation for scattered waves are shown by the arrows at A and B for ψ=0,β=4.40,κy=3.1113 and ψ=π/6,β=4.45,κy=2.225, respectively. (b) Real part of the displacement field for β=4.40, ψ=π/4, κy=3.1113 for the rectangular lattice. The Foldy method was used for 2000 gratings. (Online version in colour.)