• Laser & Optoelectronics Progress
  • Vol. 56, Issue 15, 152501 (2019)
Haojie Hou1, Junyan Liu1、2, Bowen Xiao2, Mingqi Zhu2, and Mengchun Li2、*
Author Affiliations
  • 1 Key Laboratory of Advanced Transducers and Intelligent Control System of the Ministry of Education, Taiyuan, Shanxi 0 30024, China
  • 2 College of Physics and Optoelectronics, Taiyuan University of Technology, Taiyuan, Shanxi 0 30024, China
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    DOI: 10.3788/LOP56.152501 Cite this Article Set citation alerts
    Haojie Hou, Junyan Liu, Bowen Xiao, Mingqi Zhu, Mengchun Li. Formation of Orthogonal and Parallel Surface-Lattice Resonances with Asymmetric Nanoparticle Array[J]. Laser & Optoelectronics Progress, 2019, 56(15): 152501 Copy Citation Text show less
    Optical responses of single L-shaped gold nanorod. (a) Schematic of L-shaped gold nanorod; (b) scattering spectrum of nanorod (solid line) and contribution of electric dipole scattering in x and y directions (dashed line); near-field distribution characteristics of (c) anti-bonding and (d) bonding localized surface plasmon resonances; (e) variation in scattering spectrum with length of nanorod; (f) variation in scattering spectrum with width of nanorod; (g) variation in scattering spectrum with
    Fig. 1. Optical responses of single L-shaped gold nanorod. (a) Schematic of L-shaped gold nanorod; (b) scattering spectrum of nanorod (solid line) and contribution of electric dipole scattering in x and y directions (dashed line); near-field distribution characteristics of (c) anti-bonding and (d) bonding localized surface plasmon resonances; (e) variation in scattering spectrum with length of nanorod; (f) variation in scattering spectrum with width of nanorod; (g) variation in scattering spectrum with
    Optical responses of L-shaped nanoparticle array. (a) Extinction spectrum of L-shaped nanoparticle array under normal incidence when periods in x direction are 1120 nm and 1150 nm and period in y direction is fixed at 1120 nm (inset represents diagram of L-shaped nanoparticle array); (b) transmission spectrum of L-shaped nanoparticle array versus period in x direction
    Fig. 2. Optical responses of L-shaped nanoparticle array. (a) Extinction spectrum of L-shaped nanoparticle array under normal incidence when periods in x direction are 1120 nm and 1150 nm and period in y direction is fixed at 1120 nm (inset represents diagram of L-shaped nanoparticle array); (b) transmission spectrum of L-shaped nanoparticle array versus period in x direction
    Electric field intensity distributions (upper) and field component distributions in x (middle) and y (lower) directions at different wavelengths. (a) Wavelength of 1515 nm; (b) wavelength of 1498 nm; (c) wavelength of 1542 nm
    Fig. 3. Electric field intensity distributions (upper) and field component distributions in x (middle) and y (lower) directions at different wavelengths. (a) Wavelength of 1515 nm; (b) wavelength of 1498 nm; (c) wavelength of 1542 nm
    Optical responses of L-shaped nanoparticle array. (a) Extinction spectrum of L-shaped nanoparticle array under normal incidence when periods in x direction are 670 nm and 690 nm and period in y direction is fixed at 690 nm; (b) transmission spectrum of L-shaped nanoparticle array versus period in x direction
    Fig. 4. Optical responses of L-shaped nanoparticle array. (a) Extinction spectrum of L-shaped nanoparticle array under normal incidence when periods in x direction are 670 nm and 690 nm and period in y direction is fixed at 690 nm; (b) transmission spectrum of L-shaped nanoparticle array versus period in x direction
    Electric field intensity distributions (upper) and field component distributions in x (middle) and y (lower) directions at different wavelengths. (a) Wavelength of 934 nm; (b) wavelength of 894 nm; (c) wavelength of 927 nm
    Fig. 5. Electric field intensity distributions (upper) and field component distributions in x (middle) and y (lower) directions at different wavelengths. (a) Wavelength of 934 nm; (b) wavelength of 894 nm; (c) wavelength of 927 nm
    Haojie Hou, Junyan Liu, Bowen Xiao, Mingqi Zhu, Mengchun Li. Formation of Orthogonal and Parallel Surface-Lattice Resonances with Asymmetric Nanoparticle Array[J]. Laser & Optoelectronics Progress, 2019, 56(15): 152501
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