Electrically resonant terahertz metamaterials: Theoretical and experimental investigations
By Willie J Padilla, M. Aronsson, C. Highstrete, Mark Lee, A. Taylor, R. Averitt. 2007
389 citations recorded by the source corpus.
Subfields: Electrical and Electronic Engineering, Electronic, Optical and Magnetic Materials
View Paper: https://www.semanticscholar.org/paper/0ecb89d94257f0575a6f2487675b5132efcdd03a
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Electrical and Electronic Engineering
- Houtong Chen
- Withawat Withayachumnankul
- A. Taylor
- Derek Abbott
- Willie J Padilla
- Xin Zhang
- H. Tao
- R. Averitt
In Electronic, Optical and Magnetic Materials
- Houtong Chen
- A. Taylor
- Willie J Padilla
- Derek Abbott
- Withawat Withayachumnankul
- R. Averitt
- Xin Zhang
- H. Tao
Citations in the corpus
- Recent Progress in Electromagnetic Metamaterial Devices for Terahertz Applications (2011, methodology): “by the reference yields the complex spectral transmission for the far-field characterization of the THz MMs [73], [74].”
- Progress in superconducting metamaterials (2014, background): “The realizations include (from top-to-bottom) single and double [109] split rings, two types of ASRs [21, 30], the split-cross structure [17], the woodcut flux-quantization split-ring resonator [74], the spiral [36], and rf- [83, 88], dc- [101], and multi-junction [141] SQUIDs and qubits.”
- Metantenna: When Metasurface Meets Antenna Again (2020, background): “In the way, the canonical electric resonator [8], [9] and split-ring resonator (SRR) [3] can be obtained quite naturally, as illustrated in Fig.”
- Metamaterials in the Terahertz Regime (2009, methodology): “A number of eSRRs are designed to resonate in the terahertz regime [ 30 ], [77]–[80].”
- Experimental demonstration of frequency-agile terahertz metamaterials (2008, background): “It is a variant of previously demonstrated designs[22–24] that exhibit a Lorentz-like resonant response described by a complex permittivity 2(ω) = 21+i22.”