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NANOPHOTONICS
Imaging the rainbow
Dielectric metalenses made of high-index materials can compensate material dispersion to achieve broadband
imaging in the visible.
Thomas Zentgraf
T
raditional optical lenses focus light
by altering its wavefront through
the addition of a spatially dependent
phase to the light field as it propagates
through a dispersive medium. With the
desire to integrate optical and electronic
components for applications such as
wearable optics or optical communications,
the demand for compact, lightweight, yet
high-performance optical systems is steadily
increasing. Towards this goal, in the past
few years, researchers have reported various
approaches to realize ultrathin optical
elements based on nanostructured surfaces
(metalenses), demonstrating the potential
for altering the light propagation in an
efficient and convenient way
1,2
. However,
these designs suffer from strong chromatic
aberration, making them unsuitable for
precise imaging of objects with multiple
colours. Writing in Nature Nanotechnology,
two groups now report metalens designs
that allow achromatic imaging in the visible
range
3,4
. Both groups use nanofin structures
made of high-index dielectrics to add a
spatially dependent phase to the light field.
As illustrated in Fig. 1a, a common
refractive lens made of a regular optical glass
focuses white light to different focus spots,
corresponding to the different colours,
along the propagation axis; thus resulting
in a blurred focus spot (the chromatic
aberration). The origin of this behaviour is
the dispersion of the material’s refractive
index with respect to the light wavelength,
which is inherent to all materials. In
conventional imaging systems, chromatic
aberration can be reduced by using two
lenses — one with a positive and the other
with a negative dispersion property (Fig. 1b).
These ‘achromatic’ lenses improve the
image quality when using a broadband
illumination, as the image will reconstruct
for a wide range of colours at the same plane.
Unfortunately, as demonstrated in Fig. 1,
this adds even more optical components to
the imaging system, making it heavier, larger
and more expensive — clearly not an option
for miniaturized optics.
Metalenses can potentially break this
cycle of adding more optical components to
improve the imaging quality while having
the potential of being easily integrated
into optical systems. It has been shown,
for example, that they can image objects
at single wavelengths and control beam
shapes
5,6
. Furthermore, they can be used
for holographic applications and nonlinear
optics. However, to generate high-quality
colour images, they need to work over
the entire visible wavelength range. Up to
now, metalenses have suffered from strong
chromatic aberrations in the same way as
conventional lenses do, that is, the focal
length varies with the wavelength (Fig. 1c),
only the sign of the aberrations is opposite
due to the diffractive working principle,
resulting in a shorter focal length for
longer wavelengths.
In their reports, Chen et al. and
Wang et al. show how to compensate for
the chromatic aberration of dielectric
metalenses. Chen et al. utilized a meta-atom
design consisting of two TiO
2
nanofins
spaced close to each other
3
(Fig. 2a). The
close proximity of the nanofins results in the
formation of optical modes similar to modes
found in slot waveguides. The researchers
found that such modes can be used to add an
additional phase to the wave by adjusting the
size of the two fins. As a result, the effective
optical mode possesses different fractions
in either the high-index fins or the low-
index air gap. Based on this added degree of
freedom in the design, the researchers were
able to independently control the phase and
group delay over nearly the entire visible
spectral range, and compensate for the
chromatic dispersion effect of the lens.
Wang et al. followed a slightly different
approach in that they used single GaN
nanofins as meta-atoms
4
(and inverted
versions) that support higher-order resonant
modes in each nanofin, in analogy to cavity
modes in resonators (Fig. 2b). As these
modes depend strongly on the wavelength,
the researchers were able to demonstrate
that these ‘resonator modes’ can be used
to add a wavelength-dependent phase to
compensate for the diffractive dispersion
effect of the metalens.
Uncorrected singlet metalens
Corrected singlet metalens
Singlet lens
Achromatic doublet lens
a
b
c
d
Blurred Blurred
Sharp Sharp
Fig. 1 | Focusing of white light with lenses. a, The dispersion of a regular singlet lens made of optical
glass leads to different focal distances for different wavelengths. b, Two different lenses made of
different materials (like crown and flint glasses) forming a doublet lens can compensate the
chromatic aberrations. c, Regular metalenses resemble a singlet lens and show chromatic aberrations.
d, Chromatic aberrations can now be compensated solely by design without the need for additional
materials or lenses
3,4
.
NATURE NANOTECHNOLOGY | VOL 13 | MARCH 2018 | 179–182 | www.nature.com/naturenanotechnology
© 2018 Macmillan Publishers Limited, part of Springer Nature. All rights reserved.