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Chiral Metasurfaces

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Author(s)
Jeong, Hyeon-HoEslami, SahandKim, InsookSachs, JohannesAlarcón-Correa, MarianaLee, Tung-ChunGibbs, John G.Singh, Dhruv P.Mark, Andrew G.Fischer, Peer
Type
Conference Paper
Citation
36th Progress in Electromagnetics Research Symposium (PIERS)
Issued Date
2015-07-06
Abstract
Two dimensional chiral surfaces exhibit interesting polarization properties and
can, by virtue of their additional symmetry-breaking, give rise to additional second harmonic
generation signals. Here, we describe arrays of chiral nanostructures that form metasurfaces with
dense sub-wavelength features, which can simultaneously exhibit multiple properties, including
plasmonic enhancement and very strong optical activities. These chiral metasurfaces are based
on a parallel fabrication scheme we have recently developed that allows shape-control at the
nanoscale [1]. We have grown arrays of chiral helices that predominately contain silver, gold,
copper, or oxides to name but a few of the materials. However, it is also possible to grow hybrid
structures as well as alloys or magnetic materials. The scalability of the technique is unique as
it permits the rapid structuring of nanophotonic elements at the wafer-scale.
Chiroptical responses in transmission (optical rotation) and absorption (circular dichroism) are
typically small effects. The chiroptical signal may be enhanced using amplification schemes,
including weak value amplification [2], or by increasing the multipolar light-matter interaction
itself. The latter is possible when the chiral object has a size that approaches the wavelength of
light. Since we can fabricate structures that are of a similar length-scale as the wavelength of
visible light, whilst being small enough to minimize scattering, large chiroptical signals can be
recorded even in films that are only about a 100nm thick [1]. We show chiroptical measurements
conducted on transparent substrates of wafer-scale metasurfaces [3–5]. In addition it is possible to
study the same chiral nanostructures as a colloidal suspension, a “metafluid”. Dynamic alignment
of the chiral nanocolloids permits spectral discrimination between those effects that arise in the
chiral signal due to their orientation on a chiral metasurface and those that arise in the isotropic
state.
REFERENCES
1. Mark, A. G., J. G. Gibbs, T.-C. Lee, and P. Fischer, Nat. Mater., Vol. 12, 802, 2013.
2. Pfeifer, M. and P. Fischer, Opt. Express, Vol. 19, 16508, 2011.
3. Gibbs, J. G., A. G. Mark, T.-C. Lee, S. Eslami, D. Schamel, and P. Fischer, Nanoscale, Vol. 6,
9457, 2014.
4. Gibbs, J. G., A. G. Mark, S. Eslami, and P. Fischer, Appl. Phys. Lett., Vol. 103, 213101-1–
213101-4, 2013.
5. Eslami, S. J. G. Gibbs, Y. Rechkemmer, J. van Slageren, M. Alarc´on-Correa, T.-C. Lee,
A. G. Mark, G. L. J. A. Rikken, and P. Fischer, ACS Photonics, Vol. 1, 1231–1236, 2014.
Publisher
THE ELECTROMAGNETICS ACADEMY
Conference Place
CS
URI
https://scholar.gist.ac.kr/handle/local/21332
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