2019
DOI: 10.1016/j.optcom.2019.04.086
|View full text |Cite
|
Sign up to set email alerts
|

Dynamical switching of electromagnetically induced reflectance in complementary terahertz metamaterials

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

0
6
0

Year Published

2021
2021
2023
2023

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 16 publications
(6 citation statements)
references
References 22 publications
0
6
0
Order By: Relevance
“…The real part χ r and imaginary part χ i of the susceptibility χ are related to the dispersion and the energy dissipation of the EIR system, respectively. Therefore, the reflection of the EIR metamaterial can be described as R = 1 − gχ i , where g is the geometric parameter that represents the coupling strength between the incident terahertz electric field E and the bright mode of the EIR metamaterial [36]. Subsequently, figure 4 shows the systematic tuning of the EIR metamaterial by gradually introducing the structural asymmetry.…”
Section: Resultsmentioning
confidence: 99%
“…The real part χ r and imaginary part χ i of the susceptibility χ are related to the dispersion and the energy dissipation of the EIR system, respectively. Therefore, the reflection of the EIR metamaterial can be described as R = 1 − gχ i , where g is the geometric parameter that represents the coupling strength between the incident terahertz electric field E and the bright mode of the EIR metamaterial [36]. Subsequently, figure 4 shows the systematic tuning of the EIR metamaterial by gradually introducing the structural asymmetry.…”
Section: Resultsmentioning
confidence: 99%
“…In Equation ( 8) χ r represents the dispersion. The transmittance T can be calculated by the formula T = 1 − λ 0 χ i , where χ i is proportional to the energy loss [17,36].…”
Section: Resultsmentioning
confidence: 99%
“…The tuning can be realized by changing structural parameters, using tunable materials and microelectromechanical systems (MEMS) technology. Due to the high flexibility, tunable materials-based PIT devices have become a research hotspot [17][18][19][20][21][22][23][24]. Graphene is especially widely used in the design of tunable PIT devices because of its high electron mobility, high modulation depth, tunable surface conductivity and low insertion loss characteristics.…”
Section: Introductionmentioning
confidence: 99%
“…As a similar phenomenon of EIT, the EIR effect refers to that a reflection peak appears at the position of a wider reflection spectrum 22 , 23 . The EIR effect in metamaterials can also be applied to devices such as sensing, optical switches and slow light 24 26 Moreover, the appearance of EIR effects can supplement the applications in the reflection space, while cannot be achieved based on the EIT effects in the transmission space.…”
Section: Introductionmentioning
confidence: 99%
“…22,23 The EIR effect in metamaterials can also be applied to devices such as sensing, optical switches and slow light. [24][25][26] Moreover, the appearance of EIR effects can supplement the applications in the reflection space, while cannot be achieved based on the EIT effects in the transmission space. Nevertheless, most of metamaterial structures reported so far only have single EIT effect or EIR effect, there are few designs that support both effects in terahertz (THz) band and achieve tuning characteristics.…”
Section: Introductionmentioning
confidence: 99%