2018
DOI: 10.1039/c8ra02981d
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Polarization-independent and angle-insensitive electromagnetically induced transparent (EIT) metamaterial based on bi-air-hole dielectric resonators

Abstract: We numerically demonstrate that an electromagnetically induced transparent (EIT) all-dielectric metamaterial with properties of polarization-independence and incident angle insensitivity can be achieved in terahertz regimes. The metamaterial cell is composed of two bi-air-hole cubes (BCs) with different sizes. The two BCs function as superradiant and subradiant resonators, respectively. Based on Mie-type destructive interferences between dielectric resonators, the EIT effect is induced at around 8.25 THz with … Show more

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Cited by 37 publications
(12 citation statements)
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“…The slow-light effect is an important phenomenon in EIT-like devices, and the performance is mainly measured by the group delay ( ) and group refractive index ( ), both of which are determined by the following formulae [ 28 , 29 , 30 ]: where , , , and are the transmission phase, angular frequency, light velocity in the vacuum, and the total thickness of the unit cell, respectively. The curves of the phase and group delay obtained from the present structure as a function of frequency during the growth of the graphene chemical potential from 0.6 eV to 0.7 eV in 0.025 eV increments are given in Figure 6 a–e, and it is known that the present device is capable of achieving a stable 0.6 ps group delay within the proposed chemical potential interval.…”
Section: Resultsmentioning
confidence: 99%
“…The slow-light effect is an important phenomenon in EIT-like devices, and the performance is mainly measured by the group delay ( ) and group refractive index ( ), both of which are determined by the following formulae [ 28 , 29 , 30 ]: where , , , and are the transmission phase, angular frequency, light velocity in the vacuum, and the total thickness of the unit cell, respectively. The curves of the phase and group delay obtained from the present structure as a function of frequency during the growth of the graphene chemical potential from 0.6 eV to 0.7 eV in 0.025 eV increments are given in Figure 6 a–e, and it is known that the present device is capable of achieving a stable 0.6 ps group delay within the proposed chemical potential interval.…”
Section: Resultsmentioning
confidence: 99%
“…The similar distributions can also be confirmed by the vector plot of the magnetic field, which is presented in the Supporting Information and clearly shows that two symmetrical vectors circulations of the magnetic field are clearly formed on both sides of the TiO 2 NBSRs, corresponding to the feature of the 1-order Mie magnetic resonances. [67] So that a resonant frequency with strong contrasting Q factors but small frequency detuning is produced at 0.75 THz compared to the bright resonance in Figure 2a. The Q factors of basic resonance modes are calculated as below and listed in Table 2.…”
Section: Structure Design and Numerical Analysismentioning
confidence: 94%
“…The similar distributions can also be confirmed by the vector plot of the magnetic field, which is presented in the Supporting Information and clearly shows that two symmetrical vectors circulations of the magnetic field are clearly formed on both sides of the TiO 2 NBSRs, corresponding to the feature of the 1‐order Mie magnetic resonances. [ 67 ]…”
Section: Structure Design and Numerical Analysismentioning
confidence: 99%
“…To obtain polarization-independent EIT-like devices, many complex structures have been designed 8 , 23 27 However, these structures, such as other polarization-sensitive EIT-like devices, still use the coupling effect between the transverse resonance modes to obtain the EIT effect. In fact, optical metamaterial devices not only have transverse resonance modes but also can obtain EIT-like effects using longitudinal modes 7 …”
Section: Introductionmentioning
confidence: 99%