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Controlling the Visible Electromagnetic Resonances of
Si/SiO
2
Dielectric Core–Shell Nanoparticles by Thermal
Oxidation
Yuta Tsuchimoto, Taka-aki Yano,* Masaki Hada, Kazutaka G. Nakamura,
Tomohiro Hayashi, and Masahiko Hara
suppressing quenching.
[2]
These results are promising for the
applications of dielectric nanostructures in field-enhanced
spectroscopy and imaging.
Dielectric nanoparticles have been also considered as a
good magnetic resource for the metamaterials working in the
visible spectral region. They are known to possess both elec-
tric dipole (ED) and also magnetic dipole (MD) resonances
in the visible region.
[3–6]
MDs are excited in the nanoparticles
through circulating displacement currents generated inside
the particles, and they scatter the “magnetic” light into far-
field. Fundamental characteristics of the dielectric nanostruc-
tures as a magnetic resource have been experimentally
[3,5,7]
and theoretically
[8,9]
studied. Using theoretical analysis based
on Mie theory, Si nanoparticles have been shown to exhibit
MD resonances in the visible
[4]
and infrared
[8]
regions, that
are strongly dependent on the nanoparticle size. Strong MD
responses of Si nanoparticles were experimentally observed
in the visible region of the spectrum with the use of a dark-
field optical microscope.
[3,5]
Along with the far-field studies,
the near-field characteristics of localized magnetic fields of
silicon dimmers have been investigated; in these, hot spots
derived from MDs were visualized with the use of near-field
scanning optical microscopy.
[10]
EDs and MDs excited in the dielectric nanostructures
lead to attractive scattering properties enabling us to achieve
unidirectional scattering.
[11–15]
In 1983, Kerker et al. theoreti-
cally demonstrated that dielectric particles exhibit spatially
anisotropic scattering patterns arising from interference of
EDs and MDs inside the particles.
[16]
The theory predicted
complete suppression of back scattering light from magne-
todielectric particles that have recently been experimentally
verified in the visible spectra region using Si and gallium
arsenide nanoparticles.
[11,12]
Resonant wavelengths of electric and magnetic multipoles
can be controlled by the shapes of dielectric nanostructures,
leading to tunability of spectral distances of the optical reso-
nances.
[17,18]
Laser printing of single Si nanoparticles, which
enables control of particle size and arrangement of com-
plex structures precisely, has been developed recently.
[19]
Among the dielectric nanostructures with various shapes,
core–shell nanoparticles may open up a novel way of con-
trolling the optical properties mentioned above because of
their tunability of electromagnetic resonances and scattering
directivity. Recently, several theoretical studies have been DOI: 10.1002/smll.201500884
Dielectrics
Y. Tsuchimoto, Dr. T. Yano, Prof. T. Hayashi,
Prof. M. Hara
Department of Electronic Chemistry
Tokyo Institute of Technology
Yokohama, Kanagawa 226-8503, Japan
E-mail: yano@echem.titech.ac.jp
Dr. T. Yano, Prof. T. Hayashi, Prof. M. Hara
RIKEN
2-1 Hirosawa
Wako, Saitama 351-0198, Japan
Dr. M. Hada, Prof. K. G. Nakamura
Materials and Structures Laboratory
Tokyo Institute of Technology
Nagatsuta 4259, Yokohama 226-8503, Japan
Dr. M. Hada
PRESTO
Japan Science and Technology Agency
Kawaguchi 332-0012, Japan
Prof. K. G. Nakamura
CREST
Japan Science and Technology Agency
Kawaguchi 332-0012, Japan
Prof. M. Hara
Earth-Life Science Institute
Tokyo Institute of Technology
Meguro, Tokyo 152-8551, Japan
Dielectric nanostructures with a high refractive index and a
low optical loss have attracted considerable attention as an
alternative to plasmonic nanostructures. Electromagnetic
multipoles excited in the high-index dielectric nanostructures
enable us to the manipulation of light beyond the diffraction
limit and to offer high electromagnetic field enhancement
comparable with that exhibited by the plasmonic nanostruc-
tures. In addition, these nanostructures have the remarkable
advantage of being able to suppress heat generation caused
by energy losses and quenching.
[1,2]
Recently numerical cal-
culations have demonstrated that dielectric nanoantennas
made of gallium phosphide exhibit ultra-low energy losses
with strongly enhanced electromagnetic fields in the visible
region.
[1]
An analytical model based on dipole–dipole inter-
actions has demonstrated that nanodimmers made of silicon
(Si) produce strongly localized electromagnetic field and
show a high quantum efficiency of localized emitters while
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