• Chinese Optics Letters
  • Vol. 16, Issue 5, 050002 (2018)
Quan Xu1, Xueqian Zhang1, Yuehong Xu1, Chunmei Ouyang1、*, Yanfeng Li1, Jiaguang Han1, and Weili Zhang1、2
Author Affiliations
  • 1Center for Terahertz Waves and College of Precision Instrument and Optoelectronics Engineering, Key Laboratory of Opto-electronics Information and Technical Science, Ministry of Education, Tianjin University, Tianjin 300072, China
  • 2School of Electrical and Computer Engineering, Oklahoma State University, Stillwater, Oklahoma 74078, USA
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    DOI: 10.3788/COL201816.050002 Cite this Article Set citation alerts
    Quan Xu, Xueqian Zhang, Yuehong Xu, Chunmei Ouyang, Yanfeng Li, Jiaguang Han, Weili Zhang. Near-field manipulation of terahertz surface waves by metasurfaces [Invited][J]. Chinese Optics Letters, 2018, 16(5): 050002 Copy Citation Text show less
    Schematic view of (a) single slit resonator and (b) a pair of slit resonators. (c) Calculated normalized amplitude and (d) phase distributions of the SWs excited by a pair of slit resonators at various θ1 and θ2 (here, LCP incidence was taken as an example).
    Fig. 1. Schematic view of (a) single slit resonator and (b) a pair of slit resonators. (c) Calculated normalized amplitude and (d) phase distributions of the SWs excited by a pair of slit resonators at various θ1 and θ2 (here, LCP incidence was taken as an example).
    (a) Calculated, (c) simulated, and (e) measured V-shaped SW intensity profiles (|Ez|2) rebuilt under LCP incidence, respectively. (b) Calculated, (d) simulated, and (f) measured N-shaped SW intensity profiles (|Ez|2) rebuilt under RCP incidence, respectively. Scale bar: 0.8 mm.
    Fig. 2. (a) Calculated, (c) simulated, and (e) measured V-shaped SW intensity profiles (|Ez|2) rebuilt under LCP incidence, respectively. (b) Calculated, (d) simulated, and (f) measured N-shaped SW intensity profiles (|Ez|2) rebuilt under RCP incidence, respectively. Scale bar: 0.8 mm.
    Simulated spectra and SW field distributions (|Ez|) of (a), (b) slit resonator array, (c), (d) split-ring-shaped slit resonator array, and (e), (f) coupled slit-pair resonator array under the x-polarization incidence, respectively. The insets in the top–left corner represent the corresponding unit elements similarly hereinafter. Scale bar: 1 mm.
    Fig. 3. Simulated spectra and SW field distributions (|Ez|) of (a), (b) slit resonator array, (c), (d) split-ring-shaped slit resonator array, and (e), (f) coupled slit-pair resonator array under the x-polarization incidence, respectively. The insets in the top–left corner represent the corresponding unit elements similarly hereinafter. Scale bar: 1 mm.
    (a)–(e) Simulated and (f)–(j) measured field intensity distributions (|Ez|2) of coupled slit-pair resonator-based metalens with different vertical distances, respectively, under x-polarization incidence. Scale bar: 1 mm.
    Fig. 4. (a)–(e) Simulated and (f)–(j) measured field intensity distributions (|Ez|2) of coupled slit-pair resonator-based metalens with different vertical distances, respectively, under x-polarization incidence. Scale bar: 1 mm.
    (a) Schematic and (b) sample image of the SSR pair; scale bar: 25 μm. The subscript and superscript of A represent the SW propagating direction and SSR number, respectively. (c)–(f) Measured SW field distributions in the case of the x-polarized, y-polarized, LCP, and RCP incidences, respectively. Scale bar: 1 mm.
    Fig. 5. (a) Schematic and (b) sample image of the SSR pair; scale bar: 25 μm. The subscript and superscript of A represent the SW propagating direction and SSR number, respectively. (c)–(f) Measured SW field distributions in the case of the x-polarized, y-polarized, LCP, and RCP incidences, respectively. Scale bar: 1 mm.
    Quan Xu, Xueqian Zhang, Yuehong Xu, Chunmei Ouyang, Yanfeng Li, Jiaguang Han, Weili Zhang. Near-field manipulation of terahertz surface waves by metasurfaces [Invited][J]. Chinese Optics Letters, 2018, 16(5): 050002
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