2008
DOI: 10.1103/physrevlett.101.253903
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Metamaterial Analog of Electromagnetically Induced Transparency

Abstract: We demonstrate a classical analog of electromagnetically induced transparency in a planar metamaterial. We show that pulses propagating through such metamaterials experience considerable delay. The thickness of the structure along the direction of wave propagation is much smaller than the wavelength, which allows successive stacking of multiple metamaterial slabs leading to increased transmission and bandwidth.

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Cited by 828 publications
(517 citation statements)
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“…Other more near-term applications employ the (sharp) metamaterial resonances for sensing purposes 99 via their dependence on environment or investigate nonlinear frequency conversion 6,[100][101][102][103][104][105][106] . In addition, the metamaterial analogue of electromagnetically-induced transparency (EIT) [107][108][109][110] shows a transparency window with extremely low absorption and strong adjustable dispersion. The latter could lead to "slow-light" applications from the microwave regime up to THz frequencies, where the structures can be fabricated quite easily.…”
Section: Discussionmentioning
confidence: 99%
“…Other more near-term applications employ the (sharp) metamaterial resonances for sensing purposes 99 via their dependence on environment or investigate nonlinear frequency conversion 6,[100][101][102][103][104][105][106] . In addition, the metamaterial analogue of electromagnetically-induced transparency (EIT) [107][108][109][110] shows a transparency window with extremely low absorption and strong adjustable dispersion. The latter could lead to "slow-light" applications from the microwave regime up to THz frequencies, where the structures can be fabricated quite easily.…”
Section: Discussionmentioning
confidence: 99%
“…[72][73][74][75][76][77][78][79][80] EIT was first discovered in atomic systems. In a three-level atomic EIT system, 71 the coupling between the excited energy level |2i with a dipole-allowed transition to the ground state |1i and a metastable level |3i by a control beam leads to a destructive interference ( Fig.…”
Section: Interaction Of Meta-atomsmentioning
confidence: 99%
“…If these two resonances are brought in close proximity in both the spatial and frequency domains, they can interfere resulting in an extremely narrow reflection or transmission window. Due to the low radiative loss of the dark mode, the Fano resonance can be extremely sharp, resulting in complete transmission, analogous to EIT [2][3][4][5][6][7][8][9][10] , or complete reflection 13 , from the sample across a very narrow bandwidth. However, the main limitation of metal-based Fano-resonant systems is the large non-radiative loss due to ohmic damping, which limits the achievable Q-factor 17 to oB10.…”
mentioning
confidence: 99%
“…This concept was later extended to classical optical systems using plasmonic metamaterials [2][3][4][5][6][7][8][9][10] , among others 11,12 , allowing experimental implementation with incoherent light and operation at room temperature. The transparent and highly dispersive nature of EIT offers a potential solution to the longstanding issue of loss in metamaterials as well as the creation of ultra-high-quality-factor (Q-factor) resonances, which are critical for realizing low-loss slow-light devices 2,3,6,10 , optical sensors 13,14 and enhancing nonlinear interactions 15 .…”
mentioning
confidence: 99%