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Graphene Controls Colour of Plasmonic Nanoantennas
J. Mertens1, A. L. Eiden2, C. Tserkezis3, J. Aizpurua3, A. C. Ferrari2, J. J. Baumberg1
1 NanoPhotonics
Centre, Cavendish Laboratory, Department of Physics, University of Cambridge, UK
2 Cambridge Graphene Centre, University of Cambridge, UK
3 Materials Physics Centre, Donostia-San Sebastián, Spain
Why nanoantennas?
• APPLICATIONS: Nanoantennas concentrate light in small gaps. Trapped light in the antenna provides a
nanometre-scale sensor that changes colour depending on the environment
• FUNDAMENTAL: We can observe quantum processes for gaps in the subnanometre regime using light
• light causes the electrons in
metallic nanoparticles (NPs)
to oscillate back and forth
Nanoparticle on mirror
light field
What is plasmonics?
time
oscillating
electrons
• dimer geometry is useful for surface enhanced
Raman scattering to study substances in gap
• problem: Dimers are hard to fabricate / handle
• solution: Equivalent geometry – NP on a mirror
 the particle shape and size
define the frequency of oscillation, i.e. the colour
 light is strongly enhanced in a gap
when NPs are close together (dimer geometry)
NP and its
reflection
one atomic
thin gap
• graphene: thinnest possible spacer
robust, stable, and controlled subnanometre gap
Graphene sets the colour
We observe coupling between a NP and its reflection using a microscope:
bulk graphite
white
light
dark field
microscopy
few layer
graphene
1
Scattering [normalised]
dark field scattering
spectra of single NPs on different graphene layers
0
1
monolayer
graphene
𝑺𝑷
𝑸
5 layer graphene
𝑷
𝒄𝒐𝒖𝒑𝒍𝒆𝒅
𝑺𝑷
0
500
600
700
Wavelength [nm]
800
The coupled resonance shifts with the number of graphene layers: we observe different plasmon modes
SP: single particle resonance – visible without a mirror
coupled: plasmon-image coupling – depends on junction between NP and mirror
• splitting of coupled resonance only for single graphene layer (1)
Interpretation: Plasmonic dipole coupling
The spectroscopy indicates a mixing of plasmonic dipoles:
global dipole: electron tunnelling through graphene layer (charge transfer)
gap dipole: highly localised charges at gap
• parallel and antiparallel alignment leads to different energies
• quantum mechanical effect sets splitting due to gap of 0.34 nm
P -resonance
Q -resonance
low energy
high energy
What can it be used for?
• tuning plasmon resonances: optically with semiconductor spacers (2) or electronically via gating
• non invasive optical probing of electronic and optical properties of the spacer material
(1) Mertens et al., Nano Lett., 2013, 13 (11)
(2) Sigle & Mertens et al., to be published, 2014
www.np.phy.cam.ac.uk