• Laser & Optoelectronics Progress
  • Vol. 60, Issue 19, 1925001 (2023)
Rui Jiang, Fang Chen, Zhaohui Zheng, Shaoying Ke, Jinrong Zhou, Guanzhou Liu, and Zhiwei Huang*
Author Affiliations
  • College of Physics and Information Engineering, Minnan Normal University, Zhangzhou 363000, Fujian , China
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    DOI: 10.3788/LOP221634 Cite this Article Set citation alerts
    Rui Jiang, Fang Chen, Zhaohui Zheng, Shaoying Ke, Jinrong Zhou, Guanzhou Liu, Zhiwei Huang. Simulation and Analysis of Extinction Properties of Rh Nanostructures[J]. Laser & Optoelectronics Progress, 2023, 60(19): 1925001 Copy Citation Text show less
    Cross-sectional (XZ) view of Rh nanostructure model
    Fig. 1. Cross-sectional (XZ) view of Rh nanostructure model
    Comparison of LSPR properties of Rh, Au and Ag at different wavelengths. (a) Real part of the permittivity; (b) imaginary part of the permittivity; (c) quality factors for LSPR
    Fig. 2. Comparison of LSPR properties of Rh, Au and Ag at different wavelengths. (a) Real part of the permittivity; (b) imaginary part of the permittivity; (c) quality factors for LSPR
    Simulation results of LSPR effect of Rh nanoparticles with different diameters. (a) Extinction spectra; (b) variation trend of formant under the longitudinal mode; (c) variation trend of formant under the transverse mode; (d) electric field distribution in the XY plane with a diameter of 100 nm under the transverse mode; (e) electric field distribution in the XY plane with a diameter of 100 nm under the longitudinal mode; (f) electric field distribution in the XY plane with a diameter of 140 nm under the longitudinal mode
    Fig. 3. Simulation results of LSPR effect of Rh nanoparticles with different diameters. (a) Extinction spectra; (b) variation trend of formant under the longitudinal mode; (c) variation trend of formant under the transverse mode; (d) electric field distribution in the XY plane with a diameter of 100 nm under the transverse mode; (e) electric field distribution in the XY plane with a diameter of 100 nm under the longitudinal mode; (f) electric field distribution in the XY plane with a diameter of 140 nm under the longitudinal mode
    Simulation results of LSPR effect of Rh nanoparticles at different heights. (a) Extinction spectra; (b) variation trend of formant under the longitudinal mode; (c) variation trend of formant under the the transverse mode; (d) electric field distribution in the XY plane with a height of 90 nm under the transverse mode; (e) electric field distribution in the XY plane with a height of 90 nm under the longitudinal mode; (f) electric field distribution in the XY plane with a height of 120 nm under the longitudinal mode
    Fig. 4. Simulation results of LSPR effect of Rh nanoparticles at different heights. (a) Extinction spectra; (b) variation trend of formant under the longitudinal mode; (c) variation trend of formant under the the transverse mode; (d) electric field distribution in the XY plane with a height of 90 nm under the transverse mode; (e) electric field distribution in the XY plane with a height of 90 nm under the longitudinal mode; (f) electric field distribution in the XY plane with a height of 120 nm under the longitudinal mode
    Simulation results of LSPR effect of Rh nanoparticles at different spacing.(a) Extinction spectra; (b) variation trend of formant under the longitudinal mode; (c) variation trend of formant under the transverse mode; (d) electric field distribution in the XY plane with a spacing of 100 nm under the transverse mode; (e) electric field distribution in the XY plane with a spacing of 100 nm under the longitudinal mode; (f) electric field distribution in the XY plane with a spacing of 120 nm under the longitudinal mode
    Fig. 5. Simulation results of LSPR effect of Rh nanoparticles at different spacing.(a) Extinction spectra; (b) variation trend of formant under the longitudinal mode; (c) variation trend of formant under the transverse mode; (d) electric field distribution in the XY plane with a spacing of 100 nm under the transverse mode; (e) electric field distribution in the XY plane with a spacing of 100 nm under the longitudinal mode; (f) electric field distribution in the XY plane with a spacing of 120 nm under the longitudinal mode
    Electron distribution between a pair of Rh nanoparticles. (a) Longitudinal mode; (b) transverse mode
    Fig. 6. Electron distribution between a pair of Rh nanoparticles. (a) Longitudinal mode; (b) transverse mode
    Simulation results of LSPR effect of Rh nanoparticles with different substrate refractive indices.(a) Extinction spectra; (b) variation trend of formant under the longitudinal mode; (c) electric field distribution in XY plane of substrate with refractive index of 1 under the longitudinal mode; (d) electric field distribution in XY plane of substrate with refractive index of 1.6 under the longitudinal mode
    Fig. 7. Simulation results of LSPR effect of Rh nanoparticles with different substrate refractive indices.(a) Extinction spectra; (b) variation trend of formant under the longitudinal mode; (c) electric field distribution in XY plane of substrate with refractive index of 1 under the longitudinal mode; (d) electric field distribution in XY plane of substrate with refractive index of 1.6 under the longitudinal mode
    Simulation results of LSPR effect of Rh nanoparticles under different environmental refractive indices. (a) Extinction spectra; (b) variation trend of formant under the longitudinal mode
    Fig. 8. Simulation results of LSPR effect of Rh nanoparticles under different environmental refractive indices. (a) Extinction spectra; (b) variation trend of formant under the longitudinal mode
    Rui Jiang, Fang Chen, Zhaohui Zheng, Shaoying Ke, Jinrong Zhou, Guanzhou Liu, Zhiwei Huang. Simulation and Analysis of Extinction Properties of Rh Nanostructures[J]. Laser & Optoelectronics Progress, 2023, 60(19): 1925001
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