Abstract
We show that an arbitrary body or aggregate can be made perfectly absorbing at discrete frequencies if a precise amount of dissipation is added under specific conditions of coherent monochromatic illumination. This effect arises from the interaction of optical absorption and wave interference and corresponds to moving a zero of the elastic S matrix onto the real wave vector axis. It is thus the time-reversed process of lasing at threshold. The effect is demonstrated in a simple Si slab geometry illuminated in the 500-900 nm range. Coherent perfect absorbers act as linear, absorptive interferometers, which may be useful as detectors, transducers, and switches. © 2010 The American Physical Society.
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CITATION STYLE
Chong, Y. D., Ge, L., Cao, H., & Stone, A. D. (2010). Coherent perfect absorbers: Time-reversed lasers. Physical Review Letters, 105(5). https://doi.org/10.1103/PhysRevLett.105.053901
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