2018
DOI: 10.1364/prj.6.000692
|View full text |Cite
|
Sign up to set email alerts
|

Plasmonically induced transparency in double-layered graphene nanoribbons

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

1
94
1

Year Published

2018
2018
2024
2024

Publication Types

Select...
8

Relationship

1
7

Authors

Journals

citations
Cited by 291 publications
(96 citation statements)
references
References 61 publications
1
94
1
Order By: Relevance
“…In contrast to metallic plasmons, plasmons supported by graphene (a single atomic layer of tightly structured carbon atoms formed to a symmetric hexagonal honeycomb lattice) can not only be continuously and dynamically tuned through electrostatic biasing [24,25], but also have long propagation length, which enables a new generation of restructurable plasmonic devices and, thus, provides an ideal platform to achieve active PIT [26,27]. Although various materials and designs have been used to achieve PIT in pure metal [16,[28][29][30][31] and graphene [32][33][34][35][36][37][38][39][40][41][42], or their hybrid material-based [43][44][45] systems, most of these systems can only realize single PIT effect. For example, one of the common ways to achieve PIT is to design π-shaped/ like metasurfaces [16,28,30,33,37,45].…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…In contrast to metallic plasmons, plasmons supported by graphene (a single atomic layer of tightly structured carbon atoms formed to a symmetric hexagonal honeycomb lattice) can not only be continuously and dynamically tuned through electrostatic biasing [24,25], but also have long propagation length, which enables a new generation of restructurable plasmonic devices and, thus, provides an ideal platform to achieve active PIT [26,27]. Although various materials and designs have been used to achieve PIT in pure metal [16,[28][29][30][31] and graphene [32][33][34][35][36][37][38][39][40][41][42], or their hybrid material-based [43][44][45] systems, most of these systems can only realize single PIT effect. For example, one of the common ways to achieve PIT is to design π-shaped/ like metasurfaces [16,28,30,33,37,45].…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, they only allow one bright to dark coupling pathway in one particular polarization direction, resulting in only one polarization-dependent PIT effect. Though our previous studies have demonstrated PIT systems with two bright-dark mode coupling pathways in pure graphene nanoribbons (GNRs) [35] or grating-coupled [38] structures, the tally polarization-insensitive single-window PIT or polarization-dependent double-window PIT effects in these systems strongly dependent on the particular choice of the geometrical parameters (see discussion part).…”
Section: Introductionmentioning
confidence: 99%
“…Importantly, the terahertz modulator can implement both amplitude and frequency modulation. In comparison to other graphene-based terahertz modulators [19][20][21], the amplitude modulation degree can reach 99.57%, meaning an excellent electro-optical switch can be realized, which is not available in other double-layered graphene system based on modulation of surface plasmons [23,24]. Moreover, the extinction ratio of Fano resonance can reach 99.70%, demonstrating an unparalleled electro-optical filter is implemented.…”
Section: Introductionmentioning
confidence: 90%
“…The tunable plasmonic resonances in graphene metasurfaces with various geometries have been intensively applied for significantly modulating the reflection, transmission, and absorption of light in the forms of plasmonically induced transparency (EIT) spectra and perfect absorbers. [87,89,[128][129][130][131][132][133][134][135][136][137][138][139][140]…”
Section: Tunable Plasmonic Resonances In Graphene Metasurfacesmentioning
confidence: 99%