Conference on Lasers and Electro-Optics 2010 2010
DOI: 10.1364/qels.2010.qpda5
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Coherent Perfect Absorbers: Time-reversed Lasers

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 … Show more

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Cited by 78 publications
(140 citation statements)
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“…In the broken phase (red curve), the second components of the eigenvectors are purely imaginary, and under conjugation, one of the components transforms into the other. It should be pointed out that the unusual scattering properties of the PT -symmetric medium have also been demonstrated in optics and electronics, both in theories and experiments [41,42,44,45].…”
Section: Scattering Propertiesmentioning
confidence: 94%
“…In the broken phase (red curve), the second components of the eigenvectors are purely imaginary, and under conjugation, one of the components transforms into the other. It should be pointed out that the unusual scattering properties of the PT -symmetric medium have also been demonstrated in optics and electronics, both in theories and experiments [41,42,44,45].…”
Section: Scattering Propertiesmentioning
confidence: 94%
“…Numerous intriguing optical phenomena have been observed in optical P T -symmetric systems, such as P T -symmetry phase transition and exceptional points [5][6][7][8], unidirectional invisibility [9,10], etc. Especially, an optical P T -symmetric medium can simultaneously behave as a coherent perfect absorber with 100% absorption [11][12][13][14], and as a laser oscillator [15,16] by simply adjusting the amplitudes and phases of incoming waves. Such a unique device is denoted as a CPA laser [17,18].…”
Section: Introductionmentioning
confidence: 99%
“…Such non-Hermitian potential regions 4,5 , which serve as sources and sinks for waves, respectively, can give rise to novel wave effects that are impossible to realize with conventional, Hermitian potentials. Examples of this kind, which were meanwhile also realized in the experiment [6][7][8][9][10] , are the unidirectional invisibility of a gain-loss potential 11 , devices that can simultaneously act as laser and as a perfect absorber [12][13][14] and resonant structures with unusual features like non-reciprocal light transmission 10 or loss-induced lasing [15][16][17] . In particular, systems with a so-called parity-time (PT ) symmetry 18 , where gain and loss are carefully balanced, have recently attracted enormous interest in the context of nonHermitian photonics [19][20][21][22][23][24] .…”
mentioning
confidence: 99%