2020
DOI: 10.1126/sciadv.aay1977
|View full text |Cite
|
Sign up to set email alerts
|

Transfer of orbital angular momentum of light to plasmonic excitations in metamaterials

Abstract: The emergence of the vortex beam with orbital angular momentum (OAM) has provided intriguing possibilities to induce optical transitions beyond the framework of the electric dipole interaction. The uniqueness stems from the OAM transfer from light to material, as demonstrated in electronic transitions in atomic systems. In this study, we report on the OAM transfer to electrons in solid-state systems, which has been elusive to date. Using metamaterials (periodically textured metallic disks), we show that multip… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
35
0

Year Published

2021
2021
2024
2024

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 56 publications
(35 citation statements)
references
References 36 publications
0
35
0
Order By: Relevance
“…For microwave applications, for the topological charges l0.28em=0.28em±1$l\; = \; \pm 1$, the circularly polarized waves can be used for the excitation, which exactly is what the spin–orbital conversion implies. [ 17,45 ] On the other hand, for applications where the excitations are realized by guided waves [ 29,31 ] (e.g., feeding networks at microwave frequencies and dielectric waveguides at optical frequencies), the first approach would need 4$\hskip.001pt 4$ phased wave ports, where the phases are determined by the irreps for the D4${D_4}$ group. The number of wave ports can quickly go up to M$M$ for the DM${D_M}$ (or CM${C_M}$) group.…”
Section: Symmetry Matching and Design Rulesmentioning
confidence: 99%
See 1 more Smart Citation
“…For microwave applications, for the topological charges l0.28em=0.28em±1$l\; = \; \pm 1$, the circularly polarized waves can be used for the excitation, which exactly is what the spin–orbital conversion implies. [ 17,45 ] On the other hand, for applications where the excitations are realized by guided waves [ 29,31 ] (e.g., feeding networks at microwave frequencies and dielectric waveguides at optical frequencies), the first approach would need 4$\hskip.001pt 4$ phased wave ports, where the phases are determined by the irreps for the D4${D_4}$ group. The number of wave ports can quickly go up to M$M$ for the DM${D_M}$ (or CM${C_M}$) group.…”
Section: Symmetry Matching and Design Rulesmentioning
confidence: 99%
“…[ 3–4 ] Besides the use of vortex modes in the communication between two parties in each other's far field, another important application of vortex modes is to manipulate micro‐, nano‐, and atomic systems [ 11–13 ] in the near field of vortex mode generators, e.g., microparticle trapping, [ 11–12 ] discriminating extreme subwavelength particles, [ 13 ] and inducing optical transitions beyond electric dipole interactions. [ 14–17 ]…”
Section: Introductionmentioning
confidence: 99%
“…[ 134 ] Another advantage of OAM modes in resonators originates from the sharp resonance peaks, which are much more sensitive to chiral scatterers than circularly polarized beams in free‐space. Owing to its flexible geometry, spoof LSPs have been demonstrated to generate OAM states in radiative [ 135–137 ] and confined modes [ 122 ] within compacted sizes. As shown in Figure , periodically modulated corrugation are used to convert confined OAM modes in the spoof LSP resonator into radiative vortex beams.…”
Section: Spoof Lsp Sensingmentioning
confidence: 99%
“…[5][6][7][8][9] Metamaterials, artificial materials composed of subwavelength structures, have shown characteristics such as negative refractive index, [10] negative permittivity, [11] high index, [12] chirality, [13] etc. Through metamaterial resonances, it is possible to manipulate the electric field, [14] magnetic field, [15] phase, [16] angular momentum, [17] etc. of light.…”
Section: Introductionmentioning
confidence: 99%