1.State Key Laboratory of Millimeter Waves, Southeast University, Nanjing 210096, China
2.Cooperative Innovation Centre of Terahertz Science, University of Electronic Science and Technology, Chengdu 611731, China
Professor TJ Cui, State Key Laboratory of Millimeter Waves, Southeast University, Nanjing 210096, China Email: tjcui@seu.edu.cn
纸质出版日期:2014-12,
网络出版日期:2014-10-24,
收稿日期:2014-08-12,
修回日期:2014-09-05,
录用日期:2014-09-09
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Coding metamaterials, digital metamaterials and programmable metamaterials[J]. LSA, 2014,3(4).
Cui, T. J. et al. Coding metamaterials, digital metamaterials and programmable metamaterials. Light: Science & Applications, 3, e218 (2014).
Coding metamaterials, digital metamaterials and programmable metamaterials[J]. LSA, 2014,3(4). DOI: 10.1038/lsa.2014.99.
Cui, T. J. et al. Coding metamaterials, digital metamaterials and programmable metamaterials. Light: Science & Applications, 3, e218 (2014). DOI: 10.1038/lsa.2014.99.
Metamaterials are artificial structures that are usually described by effective medium parameters on the macroscopic scale
and these metamaterials are referred to as 'analog metamaterials'. Here
we propose 'digital metamaterials' through two steps. First
we present 'coding metamaterials' that are composed of only two types of unit cells
with 0 and
π
phase responses
which we name '0' and '1' elements
respectively. By coding '0' and '1' elements with controlled sequences (i.e.
1-bit coding)
we can manipulate electromagnetic (EM) waves and realize different functionalities. The concept of coding metamaterials can be extended from 1-bit coding to 2-bit coding or higher. In 2-bit coding
four types of unit cells
with phase responses of 0
π
/2
π
and 3
π
/2
are required to mimic the '00'
'01'
'10' and '11' elements
respectively. The 2-bit coding has greater freedom than 1-bit coding for controlling EM waves. Second
we propose a unique metamaterial particle that has either a '0' or '1' response controlled by a biased diode. Based on this particle
we present 'digital metamaterials' with unit cells that possess either a '0' or '1' state. Using a field-programmable gate array
we realize digital control over the digital metamaterial. By programming different coding sequences
a single digital metamaterial has the ability to manipulate EM waves in different manners
thereby realizing 'programmable metamaterials'. The above concepts and physical phenomena are c
onfirmed through numerical simulations and experiments using metasurfaces.
codingdigitalmetamaterialmetasurfaceprogrammable
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