2014
DOI: 10.1103/physrevlett.112.143903
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Experimental Demonstration of a Coherent Perfect Absorber with PT Phase Transition

Abstract: We report the realization of a coherent perfect absorber, using a pair of passive resonators coupled to a microwave transmission line in the background, which can completely absorb light in its parity-time (PT-)symmetric phase but not in its broken phase. Instead of balancing material gain and loss, we exploit the incident waves in the open system as an effective gain so that ideal PT symmetry can be established by using only passive materials. Such a route will be effective to construct PT-symmetric metamater… Show more

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Cited by 445 publications
(311 citation statements)
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“…They also remain valid for any sign of Kerr nonlinearity and thus allow us to perform a modulational stability analysis for non-homogeneous potentials. The most appropriate context to study the MI of such solutions is that of PT -symmetric optics [6][7][8][9][10][11]14,[19][20][21][22]24 . We find that in the selffocusing regime, the waves are always unstable, whereas in the defocusing regime the instability appears for specific values of Bloch momenta.…”
Section: Discussionmentioning
confidence: 99%
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“…They also remain valid for any sign of Kerr nonlinearity and thus allow us to perform a modulational stability analysis for non-homogeneous potentials. The most appropriate context to study the MI of such solutions is that of PT -symmetric optics [6][7][8][9][10][11]14,[19][20][21][22]24 . We find that in the selffocusing regime, the waves are always unstable, whereas in the defocusing regime the instability appears for specific values of Bloch momenta.…”
Section: Discussionmentioning
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%
“…Since it is not easy to achieve PT symmetry experimentally, several ways have been proposed to avoid the use of gain in a system. For example, a system with asymmetric loss is equivalent to a PT -symmetric system with a background of uniform loss, and so no gain is required to achieve an EP [3,[21][22][23][24]. In a system with many coupled modes, the emergence of multiple EPs and their interactions can occur under system parameter variation [25][26][27].…”
Section: Introductionmentioning
confidence: 99%
“…Coherent perfect absorption in a system with an effective PT symmetry was first demonstrated experimentally using a pair of coupled microwave resonators [107]. Recently, two independent papers reported the realization of PT -symmetric laser-absorbers based on opticalfrequency waveguides [98,108].…”
Section: Pt -Symmetric Structuresmentioning
confidence: 99%