• Laser & Optoelectronics Progress
  • Vol. 56, Issue 20, 202420 (2019)
Chunlin Zhang1, Jie Liu2, Haojie Hou2, and Mengchun Li3、*
Author Affiliations
  • 1Shanxi Expressway Information Monitoring Center, Taiyuan, Shanxi 0 30024, China
  • 2Key Laboratory of Advanced Transducers and Intelligent Control System of Ministry of Education, Taiyuan University of Technology, Taiyuan, Shanxi 0 30024, China
  • 3College of Physics and Optoelectronics, Taiyuan University of Technology, Taiyuan, Shanxi 0 30024, China
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    DOI: 10.3788/LOP56.202420 Cite this Article Set citation alerts
    Chunlin Zhang, Jie Liu, Haojie Hou, Mengchun Li. Multiple Surface Lattice Resonances Generated with Noble Metallic Split-Ring Resonator Arrays[J]. Laser & Optoelectronics Progress, 2019, 56(20): 202420 Copy Citation Text show less
    Optical responses of a single gold split-ring resonator under x-polarized incidence that propagating along the z-axis. (a) Scattering spectrum of the split-ring resonator, and the inset denotes a schematic view of the split-ring resonator; near-field distributions at the center cross section of (b) electric quadrupole and (c) magnetic dipole resonances
    Fig. 1. Optical responses of a single gold split-ring resonator under x-polarized incidence that propagating along the z-axis. (a) Scattering spectrum of the split-ring resonator, and the inset denotes a schematic view of the split-ring resonator; near-field distributions at the center cross section of (b) electric quadrupole and (c) magnetic dipole resonances
    Optical response of split-ring resonator arrays. (a) Extinction spectra of perpendicular incidence of x polarization when the period along the y-axis is 1300 nm; (b) relation of extinction spectrum with periodic change along x direction
    Fig. 2. Optical response of split-ring resonator arrays. (a) Extinction spectra of perpendicular incidence of x polarization when the period along the y-axis is 1300 nm; (b) relation of extinction spectrum with periodic change along x direction
    Electric field amplitude distribution and the components of electric field intensity in x and y directions at different wavelengths. (a) 1972 nm; (b) 1968 nm; (c) 1995 nm
    Fig. 3. Electric field amplitude distribution and the components of electric field intensity in x and y directions at different wavelengths. (a) 1972 nm; (b) 1968 nm; (c) 1995 nm
    Optical response of split-ring resonator arrays. (a) Extinction spectra of perpendicular incidence of x polarization when the period along the y-axis is 720 nm; (b) relation of extinction spectrum with periodic change along x direction
    Fig. 4. Optical response of split-ring resonator arrays. (a) Extinction spectra of perpendicular incidence of x polarization when the period along the y-axis is 720 nm; (b) relation of extinction spectrum with periodic change along x direction
    Electric field amplitude distribution and the components of electric field intensity in x and y directions at different wavelengths. (a) 1095 nm; (b) 1088 nm; (c) 1128 nm
    Fig. 5. Electric field amplitude distribution and the components of electric field intensity in x and y directions at different wavelengths. (a) 1095 nm; (b) 1088 nm; (c) 1128 nm
    Chunlin Zhang, Jie Liu, Haojie Hou, Mengchun Li. Multiple Surface Lattice Resonances Generated with Noble Metallic Split-Ring Resonator Arrays[J]. Laser & Optoelectronics Progress, 2019, 56(20): 202420
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