Forward and backward propagation guided-mode waves of electric dipole resonances in an h-BN metasurface

Sheng Zhou; Sheng Zhou; Sheng Zhou; Gao Jin; Yue Zhao; Qiang Zhang; Shu Fang Fu; Xiang Guang Wang; Xuan Wang; Xuan Zhang Wang

doi:10.1364/JOSAB.500445

Journal of the Optical Society of America B
Vol. 41,
Issue 1,
pp. 15-28
(2024)
•https://doi.org/10.1364/JOSAB.500445

Forward and backward propagation guided-mode waves of electric dipole resonances in an h-BN metasurface

Sheng Zhou, Gao Jin, Yue Zhao, Qiang Zhang, Shu Fang Fu, Xiang Guang Wang, Xuan Wang, and Xuan Zhang Wang

Not Accessible

Your library or personal account may give you access

Get PDF
Email
Share
Get Citation
Copy Citation Text
Sheng Zhou, Gao Jin, Yue Zhao, Qiang Zhang, Shu Fang Fu, Xiang Guang Wang, Xuan Wang, and Xuan Zhang Wang, "Forward and backward propagation guided-mode waves of electric dipole resonances in an h-BN metasurface," J. Opt. Soc. Am. B 41, 15-28 (2024)

Export Citation
- BibTex
- Endnote (RIS)
- HTML
- Plain Text
Citation alert
Save article

Check for updates

Abstract

The generation of a backward propagation (BP) and forward propagation (FP) guided mode in a double ridge h-BN metasurface (DRM) is investigated. h-BN is a hyperbolic metamaterial with two Reststrahlen frequency bands (RBs). The incident wave can excite guided modes in DRM, where the Poynting vector parallel component of the FP mode is identical and the BP mode is opposite to that of the incident wave. Based on the optimized structure, the frequency range of the BP mode for TE waves was found near the type II hyperbolic band (HB II), while for TM waves, it was found in the gap between the range of HB I and HB II in h-BN. To comprehensively understand the physics underlying BP and FP modes, we present the electric and magnetic field intensities in DRM, the electric field profile of beam steering, and the radiated powers of multipole resonances. The electric dipole (ED) moment contributes most significantly to the FP and BP modes, with its power being much greater than that of other multipolar moment modes. A proportion of BP mode power and incident power decreases with increasing incident angle of TE waves. There are two peaks of the proportion with TM waves. The maximum proportion is near 75% ofTE waves and 16% ofTM waves. The DRM has shown promising potential in the field of sensors based on BP mode, with a sensitivity of 3.9675 µm/RIU of TE waves and 5.1479 µm/RIU of TM waves. These findings suggest that DRMs hold significant promise for the development of optical metasurfaces, optical switches, and high-performance sensors.

Full Article | PDF Article

More Like This

Guided-mode waves structure of electric and magnetic dipole resonances in a metamaterial slab

Minyeong Kim, Eui Sun Hwang, Oleg Prudnikov, and Byoung-Ho Cheong
Opt. Express 29(19) 30610-30624 (2021)

Actively tunable terahertz metasurface absorber due to surface phonon polaritons

Feng Wei Gao, Chao Sui, Sheng Zhou, Shu Fang Fu, Xuan Wang, Yu Ling Song, Qiang Zhang, Hong Liang, and Xuan Zhang Wang
J. Opt. Soc. Am. B 39(4) 1195-1202 (2022)

Ghost surface polaritons in naturally uniaxial hyperbolic materials

Xiang-Guang Wang, Shao-Peng Hao, Shu-Fang Fu, Qiang Zhang, and Xuan-Zhang Wang
J. Opt. Soc. Am. B 40(7) 1667-1673 (2023)

Previous Article Next Article

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.

Cited By

You do not have subscription access to this journal. Cited by links are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Figures (15)

You do not have subscription access to this journal. Figure files are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Tables (1)

You do not have subscription access to this journal. Article tables are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Equations (13)

You do not have subscription access to this journal. Equations are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

No.	Published Sensors (Year Published)	Material	Size	Refractive Index (Permittivity)	Wavelength (µm) (Frequency)	Max Sensitivity (µm/RIU)
1	$G_{3} {B N}_{2}$ ribbon (2019) [17]	Graphene/h-BN	240 nm $*$ 352 nm	1.0–2.0 (1.0–4.0)	6.8, 10.3	3.1, 4.2
					44.1,29.1 THz
2	GHSHPRW (2021) [35]	h-BN/graphene	150 µm $*$ 500 nm	1.0–1.41 (1–1.98)	1.46–1.56	0.34940
	GHSHPRW (2021) [35]	h-BN/graphene	150 µm $*$ 500 nm	1.0–1.41 (1–1.98)	(192.2–205.3 THz)	0.34940
3	h-BN/graphene heterostructure (2022) [36]	$h - B N / g r a p h e n e / {C a F}_{2}$	2.5 µm $*$ 1.6 µm	1.33, 1.52 (1.77,2.31)	6.43 (46.62 THz)	0.3606, 0.3134
	h-BN/graphene heterostructure (2022) [36]	$h - B N / g r a p h e n e / {C a F}_{2}$	2.5 µm $*$ 1.6 µm	1.33, 1.52 (1.77,2.31)	6.56 (45.7 THz)	0.3606, 0.3134
4	Patterned $g r a p h e n e / {S i O}_{2} - S i$ substrate (2020) [37]	$G r a p h e n e / {S i O}_{2} / S i$	6 µm $*$ 6 µm	1.0–1.3 (1–1.69)	25–125 (2.39–11.9 THz)	13.670
5	Asymmetric resonant compound grating (2023) [38]	$S i / {S i O}_{2}$	750 nm $*$ 370 nm	1.331–1.339 (1.77–1.79)	1.252–1.262 (237.55–239.45 THz)	0.4801
6	Split-disk (2023) [39]	$S i / {S i}_{3} N_{4}$	1200 nm $*$ 1600 nm	1.33–1.41 (1.77–1.98)	2.3–2.4 (124.9–130.34 THz)	0.746
7	Two GaP $c u b o i d s / {S i O}_{2}$ substrate (2023) [40]	$G a P / {S i O}_{2}$	310 nm $*$ 310 nm	1.0–1.3 (1.0–1.69)	0.612–0.620 (483.54–491.46 THz)	0.135 (x-polarized)
	Two GaP $c u b o i d s / {S i O}_{2}$ substrate (2023) [40]	$G a P / {S i O}_{2}$	310 nm $*$ 310 nm	1.0–1.3 (1.0–1.69)	0.612–0.620 (483.54–491.46 THz)	0.045 (y-polarized)
8	h-BN ribbon (this work)	h-BN	4 µm $*$ 1.5 µm	1.33–1.36 (1.77–1.86)	6.97–7.49 (40–43 THz)	3.9675 (TE wave)
	h-BN ribbon (this work)	h-BN	4 µm $*$ 1.5 µm	1.33–1.36 (1.77–1.86)	6.97–7.49 (40–43 THz)	5.1479 (TM wave)

Abstract

Data availability

Cited By

Figures (15)

Tables (1)

Equations (13)

Journal of the Optical Society of America B