Fig. 2. (a) Effective impedance of the HMM absorber for both the amorphous (blue line) and crystalline (red line) states. (b and c) E-field intensity (left column) and absorbed power (right column) distributions of the HMM absorber for (b) the amorphous state at λa = 1180 nm, and (c) the crystalline state at λc = 1680 nm. The white arrows represent the Poynting vectors. The different regions of air and HMM are circled by the black dotted line.
