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A controlled launch for plasmons

To create nanophotonic devices, engineers must combine large-scale optics with tiny nanoelectronics. Plasmons, the collective light-induced excitations of electrons at a metal's surface, can bridge that difference in size scales. Alonso-Gonzalez et al. placed structured gold “antennas” on top of a graphene layer to launch and propagate plasmonic excitations into the graphene. By carefully designing the antennas, the researchers could engineer the wavefronts of the plasmons and control the direction of propagation. This approach illustrates a versatile approach for the development of nanophotonics.
Science, this issue p. 1369

Abstract

Graphene plasmons promise unique possibilities for controlling light in nanoscale devices and for merging optics with electronics. We developed a versatile platform technology based on resonant optical antennas and conductivity patterns for launching and control of propagating graphene plasmons, an essential step for the development of graphene plasmonic circuits. We launched and focused infrared graphene plasmons with geometrically tailored antennas and observed how they refracted when passing through a two-dimensional conductivity pattern, here a prism-shaped bilayer. To that end, we directly mapped the graphene plasmon wavefronts by means of an imaging method that will be useful in testing future design concepts for nanoscale graphene plasmonic circuits and devices.
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Supplementary Material

Summary

Materials and Methods
Figs. S1 and S2
References (3235)

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References and Notes

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Science
Volume 344 | Issue 6190
20 June 2014

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Received: 11 March 2014
Accepted: 8 May 2014
Published in print: 20 June 2014

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Acknowledgments

We thank P. S. Carney, A. Kuzmenko, I. Nechaev, and F. Guinea for stimulating discussions. Supported by the European Union through ERC starting grants (TERATOMO, SPINTROS and CarbonLight), NMP (HINTS and Grafol), Marie Curie Career Integration Grants (ITAMOSCINOM and GRANOP); the European Commission under Graphene Flagship (contract no. CNECT-ICT-604391); the Spanish Ministry of Economy and Competitiveness (National Projects MAT2012-36580 and MAT2012-37638) and from the Basque Government (Project PI2011-1). F.K. acknowledges support from the Fundacio Cellex Barcelona. R.H. is co-founder of Neaspec GmbH, a company producing scattering-type scanning near-field optical microscope systems such as the one used in this study. All other authors declare no competing financial interests.

Authors

Affiliations

P. Alonso-González
CIC nanoGUNE, 20018 Donostia-San Sebastián, Spain.
A. Y. Nikitin
CIC nanoGUNE, 20018 Donostia-San Sebastián, Spain.
IKERBASQUE, Basque Foundation for Science, 48011 Bilbao, Spain.
F. Golmar
CIC nanoGUNE, 20018 Donostia-San Sebastián, Spain.
I.N.T.I.-CONICET and ECyT-UNSAM, San Martín, Buenos Aires, Argentina.
A. Centeno
Graphenea SA, 20018 Donostia-San Sebastián, Spain.
A. Pesquera
Graphenea SA, 20018 Donostia-San Sebastián, Spain.
S. Vélez
CIC nanoGUNE, 20018 Donostia-San Sebastián, Spain.
J. Chen
CIC nanoGUNE, 20018 Donostia-San Sebastián, Spain.
G. Navickaite
ICFO-Institut de Ciéncies Fotoniques, Mediterranean Technology Park, 08860 Casteldefells, Barcelona, Spain.
F. Koppens
ICFO-Institut de Ciéncies Fotoniques, Mediterranean Technology Park, 08860 Casteldefells, Barcelona, Spain.
A. Zurutuza
Graphenea SA, 20018 Donostia-San Sebastián, Spain.
F. Casanova
CIC nanoGUNE, 20018 Donostia-San Sebastián, Spain.
IKERBASQUE, Basque Foundation for Science, 48011 Bilbao, Spain.
L. E. Hueso
CIC nanoGUNE, 20018 Donostia-San Sebastián, Spain.
IKERBASQUE, Basque Foundation for Science, 48011 Bilbao, Spain.
R. Hillenbrand* [email protected]
IKERBASQUE, Basque Foundation for Science, 48011 Bilbao, Spain.
CIC nanoGUNE and UPV/EHU, 20018 Donostia-San Sebastián, Spain.

Notes

*Corresponding author. E-mail: [email protected]

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