Author Affiliations
1Shanghai Key Lab of Modern Optical System, Engineering Research Center of Optical Instrument and System, Ministry of Education, University of Shanghai for Science and Technology, 516 Jungong Road, Shanghai 200093, China2Centre for THz Research, China Jiliang University, Hangzhou 310018, Chinashow less
Fig. 1. (a) Structural parameters and features of Dual_CSRRs, (b) microscope image of fabricated Dual_CSRRs sample, (c) shift motion of the inner resonator in CSRR-L.
Fig. 2. Simulation and measurement results of Dual_CSRRs devices with different shifting position of SRRIs: (a–c) simulated transmission spectra of devices, (d–f) measured transmission of THz wave. The inserts from top to bottom are microscope images of the fabricated Dual_CSRRs(0,0), Dual_CSRRs(30,−30), and Dual_CSRRs(40,−40), respectively.
Fig. 3. (a) Simulation results of transmission spectra for CSRR-L with Δh changing from −40 to 40 μm, (b–d) simulated transmission spectra of Dual_CSRRs and their individual CSRR-L and CSRR-R: (b) Dual_CSRRs(0,0), (c) Dual_CSRRs(30,−30), (d) Dual_CSRRs(40,−40).
Fig. 4. (a) Simulated amplitude transmission of CSRR-L, SRRI, and SRRO. (b,c) Schematics of metamaterial unit cell for SRRI and SRRO. Electric polarization is parallel to the split gap for CSRR-L and SRRI, and simulation results with polarization along both x axis and y axis for SRRO are presented.
Fig. 5. Surface current and electric field distributions of devices: (a,b) surface current distributions of CSRR-L with black arrows representing the trend of surface current on SRRIs and SRROs. (c–f) Distributions of electric field for CSRR-L and Dual_CSRRs, respectively. The frequency resonance in (a), (c), and (e) is at 0.25 THz, and the frequency resonance in (b), (d), and (f) is at 0.3 THz.
Fig. 6. Simulated transmission spectrum of Dual_CSRR(40,40) when E polarization is along the x axis; the insert is a schematic of Dual_CSRR(40,40).