scholarly journals Tunable electromagnetically induced transparency in coupled three-dimensional split-ring-resonator metamaterials

2016 ◽  
Vol 6 (1) ◽  
Author(s):  
Song Han ◽  
Longqing Cong ◽  
Hai Lin ◽  
Boxun Xiao ◽  
Helin Yang ◽  
...  
2020 ◽  
Vol 10 (15) ◽  
pp. 5267 ◽  
Author(s):  
Yuhang Liao ◽  
Yu-Sheng Lin

We propose a reconfigurable terahertz (THz) metamaterial (RTM) to investigate its multifunctional electromagnetic characteristics by moving the meta-atoms of split-ring resonator (SRR) array. It shows the preferable and capable adjustability in the THz frequency range. The electromagnetic characteristics of the proposed RTM device are compared and analyzed by moving the meta-atoms in different polarized transverse magnetic (TM) and transverse electric (TE) modes. The symmetrical meta-atoms of RTM device exhibit a resonant tuning range of several tens of GHz and the asymmetrical meta-atoms of RTM device exhibit the better tunability. Therefore, an RTM device with reconfigurable meta-atoms possesses the resonance shifting, polarization switching, electromagnetically induced transparency (EIT) switching and multiband to single-band switching characteristics. This proposed RTM device provides the potential possibilities for the use of THz-wave optoelectronics with tunable resonance, EIT analog and tunable multiresonance characteristics.


2015 ◽  
Vol 355 ◽  
pp. 337-341 ◽  
Author(s):  
Chuanqi Li ◽  
Lei Huang ◽  
Wenyan Wang ◽  
Xiangjun Ma ◽  
Shengbang Zhou ◽  
...  

2018 ◽  
Vol 32 (04) ◽  
pp. 1850030 ◽  
Author(s):  
Feng Xue ◽  
Shao-Bin Liu ◽  
Hai-Feng Zhang ◽  
Yong-Diao Wen ◽  
Xiang-Kun Kong ◽  
...  

In this paper, a tunable electromagnetically induced transparency (EIT) based on S-PINs is theoretically analyzed. Unit cell of the structure consists of a cutwire (CW), split ring resonator (SRR), and solid state plasma (SS plasma) patches which are composed of S-PIN array. The destructive interference between the CW and SRR results in a narrowband transparency window accompanied with strong phase dispersion. The proposed design can obtain a tunable EIT with different frequencies range from 12.8 GHz to 16.5 GHz in a simple method by switching these S-PINs on or off selectively. The related parameters of the S-PIN such as the size, carrier concentration, and volt-ampere characteristics have been studied theoretically. The interaction and coupling between two resonators are investigated in detail by the analysis of the current distribution and E-field strength as well. The research results provide an effective way to realize reconfigurable compact slow-light devices.


2015 ◽  
Vol 15 (3) ◽  
pp. 2289-2293 ◽  
Author(s):  
David Shawn Wilbert ◽  
Mohammad Parvinnezhad Hokmabadi ◽  
Patrick Kung ◽  
Seongsin Margaret Kim

2014 ◽  
Author(s):  
Pin Chieh Wu ◽  
Wei Ting Chen ◽  
Yao-Wei Huang ◽  
Wei-Lun Hsu ◽  
Chun Yen Liao ◽  
...  

Sensors ◽  
2018 ◽  
Vol 18 (9) ◽  
pp. 3049 ◽  
Author(s):  
Ahmed Salim ◽  
Saptarshi Ghosh ◽  
Sungjoon Lim

In this paper, a microwave cavity resonator is presented for chemical sensing applications. The proposed resonator is comprised of a three dimensional (3D) split-ring resonator (SRR) residing in an external cavity and capacitively coupled by a pair of coaxial probes. 3D-printing technology with polylactic acid (PLA) filament is used to build the 3D SRR and cavity. Then, the surfaces of the SRR and the inside walls of cavity are silver-coated. The novelty of our proposed structure is its light weight and inexpensive design, owing to the utilization of low density and low-cost PLA. A Teflon tube is passed through the split-gap of the SRR so that it is parallel to the applied electric field. With an empty tube, the resonance frequency of the structure is measured at 2.56 GHz with an insertion loss of 13.6 dB and quality factor (Q) of 75. A frequency shift of 205 MHz with respect to the empty channel was measured when deionized water (DIW) was injected into the tube. Using volume occupied by the structure, the weight of the proposed microwave resonator is estimated as 22.8 g which is significantly lighter than any metallic structure of comparable size.


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