Skip to main content
. 2015 Jun 26;6:7507. doi: 10.1038/ncomms8507

Figure 1. Frequency-dependent directional angles of the hyperbolic polaritons propagating inside the hBN.

Figure 1

Solid lines in (a,b) the critical angle θ of the HPs as a function of the frequency ω in the Type-I (760<ω<825 cm−1, ɛt>0 and ɛz<0) and Type-II (1,360<ω<1,610 cm−1, ɛt<0 and ɛz>0) hyperbolic bands of the hBN. (ch) Simulated electric-field distribution (|Ez|) at various frequencies. The directional angles evaluated from these simulations are plotted in a,b (colour dots) for comparison: θ=16° (c, at ω=761 cm−1), θ=2° (f, at ω=1,613.8 cm−1), θ=45° (d,g; at ω=778.2 cm−1 and ω=1,527 cm−1) and θ=60° (e,h; at ω=795 cm−1 and ω=1,459.6 cm−1). Scale bar, 1 μm (c).