2015
DOI: 10.1063/1.4916189
|View full text |Cite
|
Sign up to set email alerts
|

Magnetic metamaterial analog of electromagnetically induced transparency and absorption

Abstract: Articles you may be interested in Tailoring dual-band electromagnetically induced transparency in planar metamaterials J. Appl. Phys. 117, 043107 (2015); 10.1063/1.4906853Actively bias-controlled metamaterial to mimic and modulate electromagnetically induced transparency Appl. Phys. Lett.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3

Citation Types

0
21
1

Year Published

2016
2016
2024
2024

Publication Types

Select...
9

Relationship

2
7

Authors

Journals

citations
Cited by 51 publications
(22 citation statements)
references
References 25 publications
0
21
1
Order By: Relevance
“…11,12 This physical insight leads to the realization of the EIT analogues in a series of classical optical systems, such as coupled microresonators, [13][14][15] photonic crystal waveguides, 16,17 a waveguide side-coupled to resonators 18,19 and metamaterials [20][21][22] , which are robust and free from the scathing experimental requirements of quantum optics. In particular, the metamaterial analogues of EIT through the near field coupling between the bright and dark mode resonators, have enabled the realization of this phenomenon at frequencies in radiofrequency (RF), [23][24][25][26] terahertz (THz), [27][28][29][30][31][32] near-infrared [33][34][35][36] and visible regimes [38][39][40] through defining a correspondingly tailored geometry for the unit cell. Due to the subwavelength thickness, these EIT analogues with the accompanying slow light and enhanced nonlinear effects have shown great prospects in designing very compact devices, such as optical filters, 41,42 optical buffers 43,44 and ultrasensitive biosensors.…”
Section: Introductionmentioning
confidence: 99%
“…11,12 This physical insight leads to the realization of the EIT analogues in a series of classical optical systems, such as coupled microresonators, [13][14][15] photonic crystal waveguides, 16,17 a waveguide side-coupled to resonators 18,19 and metamaterials [20][21][22] , which are robust and free from the scathing experimental requirements of quantum optics. In particular, the metamaterial analogues of EIT through the near field coupling between the bright and dark mode resonators, have enabled the realization of this phenomenon at frequencies in radiofrequency (RF), [23][24][25][26] terahertz (THz), [27][28][29][30][31][32] near-infrared [33][34][35][36] and visible regimes [38][39][40] through defining a correspondingly tailored geometry for the unit cell. Due to the subwavelength thickness, these EIT analogues with the accompanying slow light and enhanced nonlinear effects have shown great prospects in designing very compact devices, such as optical filters, 41,42 optical buffers 43,44 and ultrasensitive biosensors.…”
Section: Introductionmentioning
confidence: 99%
“…The similar coherence and interference phenomenon, named as EIT-like effect, has been demonstrated in the classical systems such as plasma [14][15][16], mechanical or electric oscillators [17,18], coupled optical resonators [19][20][21][22][23][24], optical parametric oscillators [25][26][27], optomechanical systems [28][29][30] and even some metamaterial configurations [31][32][33]. Especially, the analog of EIT in coupled optical resonators, also called coupled-resonatorinduced transparency, has made great progress in experiment, which has been reported in the different optical systems, such as compound glass waveguide platform using relatively large resonators [34], fiber ring resonators [35], coupled fused-silica microspheres [36,37], integrated micron-size silicon optical resonator systems [38][39][40][41], photonic crystal cavities [42] and graphene-ring resonators [43].…”
mentioning
confidence: 56%
“…The first approach is to design two sub-structures in the micro unit of metamaterial. Two sub-structures work as bright and dark modes, respectively, where the bright mode is coupled directly with the incident wave, and the dark mode is indirectly excited by incident wave through near-field coupling with bright mode [14,[19][20][21][22][23][24]. This coupling between bright and dark modes produces an EIT effect.…”
Section: Introductionmentioning
confidence: 99%