Dual-mode bidirectional multifunctional chiral metamaterial based on self-complementary resonators

Yuxin Wang; Rongcao Yang; Rongcao Yang; Yijia Zhao; Jinping Tian; Wenmei Zhang; Li Ding; Li Ding

doi:10.1364/JOSAB.487386

Journal of the Optical Society of America B
Vol. 40,
Issue 6,
pp. 1435-1442
(2023)
•https://doi.org/10.1364/JOSAB.487386

Dual-mode bidirectional multifunctional chiral metamaterial based on self-complementary resonators

Yuxin Wang, Rongcao Yang, Yijia Zhao, Jinping Tian, Wenmei Zhang, and Li Ding

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Yuxin Wang, Rongcao Yang, Yijia Zhao, Jinping Tian, Wenmei Zhang, and Li Ding, "Dual-mode bidirectional multifunctional chiral metamaterial based on self-complementary resonators," J. Opt. Soc. Am. B 40, 1435-1442 (2023)

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Abstract

In this paper, we propose an intrinsic chiral metamaterial (ICM) consisting of two metal self-complementary resonators, dielectric layer, and an embedded continuous vanadium dioxide (${{\rm VO}_2}$) layer, which can operate in reflection and transmission modes and tailor different polarization manipulations for circular and linear polarized waves in opposite incident directions. When ${{\rm VO}_2}$ is in metallic state, the ICM can achieve broadband and narrowband circular polarization conversions at 1.52–2.50 THz and 2.93 THz for opposite propagating directions, respectively; when ${{\rm VO}_2}$ is in an insulating state, it shows a strong asymmetric transmission (AT) effect at 2.43 and 3.19 THz for forward and backward linear polarized waves. In addition, the physical mechanisms of different polarization operations are explained by analyzing the surface current and electric field distributions, multiple interference model, and near-field distributions in detail, and the circuit models are introduced to verify the simulated results. Furthermore, we investigate the influence of structural parameters on performance. The proposed ICM has important implications for the development of polarization detectors, frequency selectors, etc.

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Data availability

Data underlying the results presented in this paper are not publicly available at this time but may be obtained from the authors upon reasonable request.

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	Forward	Backward
Reflection mode	$R_{1} = 350 Ω$ , $L_{1} = 46.27 p H$ , $C_{1} = 0.05 f F$ , $R_{2} = 226 Ω$ , $L_{2} = 40.3 p H$ , $C_{2} = 0.175 f F$ , $C = 12.77 f F$ , $Z_{1} = 128.5 Ω$ , $E_{1} = {95.4}^{\circ}$ , $F_{1} = 2.211 T H z$ .	$R_{3} = 510 Ω$ , $L_{3} = 12.785 p H$ , $C_{3} = 1.2 f F$ , $C^{'} = 14 f F$ , $Z_{2} = 31 Ω$ , $E_{2} = 84^{\circ}$ , $F_{2} = 2.686 T H z$ .
Transmission mode	$R_{4} = 37.5 Ω$ , $L_{4} = 0.87 p H$ , $C_{4} = 0.165 f F$ , $C^{''} = 0.138 f F$ , $R_{5} = 2.25 Ω$ , $L_{5} = 2.82 p H$ , $C_{5} = 0.24 f F$ , $Z_{3} = 150 Ω$ , $E_{3} = {137.6}^{\circ}$ , $F_{3} = 2.46 T H z$ .	$R_{4} = 2.59 Ω$ , $L_{4} = 2.108 p H$ , $C_{4} = 0.14 f F$ , $C^{''} = 0.116 f F$ , $R_{5} = 9.11 Ω$ , $L_{5} = 7.67 p H$ , $C_{5} = 1.365 f F$ , $Z_{3} = 150 Ω$ , $E_{3} = 216^{\circ}$ , $F_{3} = 3.12 T H z$ .

Refs.	Operating Mode	Function	Frequency	Tunable Materials
[11]	Transmission	AT	1.92–1.96 THz	${V O}_{2}$
[19]	Transmission	AT	1.67–2.05 THz	${V O}_{2}$
[21]	Reflection	PC^a	3.75–6 THz	Graphene
[24]	Reflection	Abs^b	4.25–7.65 THz	Graphene
[24]	Reflection	PC	2.22–6.09 THz	Graphene
This work	Reflection Transmission	PC	1.52–2.50 THz & 2.93 THz	${V O}_{2}$
This work	Reflection Transmission	AT	2.43 & 3.19 THz	${V O}_{2}$

	Forward	Backward
Reflection mode	$R_{1} = 350 Ω$ , $L_{1} = 46.27 p H$ , $C_{1} = 0.05 f F$ , $R_{2} = 226 Ω$ , $L_{2} = 40.3 p H$ , $C_{2} = 0.175 f F$ , $C = 12.77 f F$ , $Z_{1} = 128.5 Ω$ , $E_{1} = {95.4}^{\circ}$ , $F_{1} = 2.211 T H z$ .	$R_{3} = 510 Ω$ , $L_{3} = 12.785 p H$ , $C_{3} = 1.2 f F$ , $C^{'} = 14 f F$ , $Z_{2} = 31 Ω$ , $E_{2} = 84^{\circ}$ , $F_{2} = 2.686 T H z$ .
Transmission mode	$R_{4} = 37.5 Ω$ , $L_{4} = 0.87 p H$ , $C_{4} = 0.165 f F$ , $C^{''} = 0.138 f F$ , $R_{5} = 2.25 Ω$ , $L_{5} = 2.82 p H$ , $C_{5} = 0.24 f F$ , $Z_{3} = 150 Ω$ , $E_{3} = {137.6}^{\circ}$ , $F_{3} = 2.46 T H z$ .	$R_{4} = 2.59 Ω$ , $L_{4} = 2.108 p H$ , $C_{4} = 0.14 f F$ , $C^{''} = 0.116 f F$ , $R_{5} = 9.11 Ω$ , $L_{5} = 7.67 p H$ , $C_{5} = 1.365 f F$ , $Z_{3} = 150 Ω$ , $E_{3} = 216^{\circ}$ , $F_{3} = 3.12 T H z$ .

Refs.	Operating Mode	Function	Frequency	Tunable Materials
[11]	Transmission	AT	1.92–1.96 THz	${V O}_{2}$
[19]	Transmission	AT	1.67–2.05 THz	${V O}_{2}$
[21]	Reflection	PC^a	3.75–6 THz	Graphene
[24]	Reflection	Abs^b	4.25–7.65 THz	Graphene
[24]	Reflection	PC	2.22–6.09 THz	Graphene
This work	Reflection Transmission	PC	1.52–2.50 THz & 2.93 THz	${V O}_{2}$
This work	Reflection Transmission	AT	2.43 & 3.19 THz	${V O}_{2}$

Abstract

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Equations (4)

Journal of the Optical Society of America B