• Opto-Electronic Advances
  • Vol. 5, Issue 7, 200097 (2022)
Peilong Hong1、*, Lei Xu2、*, and Mohsen Rahmani2
Author Affiliations
  • 1School of Optoelectronic Science and Engineering, University of Electronic Science and Technology of China (UESTC), Chengdu 611731, China
  • 2Advanced Optics & Photonics Laboratory, Department of Engineering, School of Science & Technology, Nottingham Trent University, Nottingham NG11 8NS, UK
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    DOI: 10.29026/oea.2022.200097 Cite this Article
    Peilong Hong, Lei Xu, Mohsen Rahmani. Dual bound states in the continuum enhanced second harmonic generation with transition metal dichalcogenides monolayer[J]. Opto-Electronic Advances, 2022, 5(7): 200097 Copy Citation Text show less
    Photonic grating slab with a pair of BICs for enhancing SHG. (a) Photonic grating slab that contains TE-type and TM-type BICs. (b) Spatial distribution of the electric field of TE and TM modes in a unit cell at Kx = 0, respectively. (c) Band structure of the target TE and TM modes of the photonic grating slab with thickness t = 0.37 ·a, respectively. (d) Kx dependent quality factor of the TE and TM modes shown in (c), respectively.
    Fig. 1. Photonic grating slab with a pair of BICs for enhancing SHG. (a) Photonic grating slab that contains TE-type and TM-type BICs. (b) Spatial distribution of the electric field of TE and TM modes in a unit cell at Kx = 0, respectively. (c) Band structure of the target TE and TM modes of the photonic grating slab with thickness t = 0.37 ·a, respectively. (d) Kx dependent quality factor of the TE and TM modes shown in (c), respectively.
    Spatial overlap coefficient and SHG efficiency with a homogeneous WS2 on top of the photonic grating slab. (a) The Kx dependent spatial overlap coefficient Z2ω,ωTMD. (b) The Kx dependent SHG efficiency monitored at the reflected (top) and transmitted (bottom) side, respectively. The blue star is a reference point for showing the SHG efficiency with a freely-standing WS2 monolayer. The FW is incident from the top side of the grating, and the intensity of FW is set to be 0.1 GW/cm2.
    Fig. 2. Spatial overlap coefficient and SHG efficiency with a homogeneous WS2 on top of the photonic grating slab. (a) The Kx dependent spatial overlap coefficient Z2ω,ωTMD. (b) The Kx dependent SHG efficiency monitored at the reflected (top) and transmitted (bottom) side, respectively. The blue star is a reference point for showing the SHG efficiency with a freely-standing WS2 monolayer. The FW is incident from the top side of the grating, and the intensity of FW is set to be 0.1 GW/cm2.
    Spatial overlap coefficient and SHG efficiency with a patterned WS2 on top of the photonic grating slab. (a) The Kx dependent spatial overlap coefficient Z2ω,ωTMD. (b) The Kx dependent SHG efficiency monitored at the reflected (top) and transmitted (bottom) side, respectively. The blue star is a reference point for showing the maximum SHG efficiency achieved in the case with homogeneous WS2 monolayer. The FW is incident from the top side of the grating, and the intensity of FW is set to be 0.1 GW/cm2.
    Fig. 3. Spatial overlap coefficient and SHG efficiency with a patterned WS2 on top of the photonic grating slab. (a) The Kx dependent spatial overlap coefficient Z2ω,ωTMD. (b) The Kx dependent SHG efficiency monitored at the reflected (top) and transmitted (bottom) side, respectively. The blue star is a reference point for showing the maximum SHG efficiency achieved in the case with homogeneous WS2 monolayer. The FW is incident from the top side of the grating, and the intensity of FW is set to be 0.1 GW/cm2.
    Peilong Hong, Lei Xu, Mohsen Rahmani. Dual bound states in the continuum enhanced second harmonic generation with transition metal dichalcogenides monolayer[J]. Opto-Electronic Advances, 2022, 5(7): 200097
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