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REVIEW
Micro- and Nanostructured Surfaces for Selective
Solar Absorption
Iryna E. Khodasevych,* Liping Wang, Arnan Mitchell, and Gary Rosengarten
DOI: 10.1002/adom.201500063
1. Introduction
Applications utilizing solar energy are being actively developed
due to increasing demand for environmentally friendly and
sustainable energy solutions. The sun is a source of tremen-
dous energy spanning from ultraviolet to infrared wavelengths,
with the maximum energy in the visible range, corresponding
to a blackbody temperature of 5780 K.
[1]
It is estimated that the
amount of solar energy reaching Earth's surface is enough to
Efficient absorption of solar radiation is desired for the renewable energy
sector, such as solar thermophotovoltaics and solar thermal applications.
In order to minimize thermal re-radiation, wavelength-selective devices are
required. Absorbers with structured surfaces are attractive because they
derive their electromagnetic properties to a greater extent from their geometry
and to a lesser extent from the intrinsic properties of the constituent mate-
rials. Thus, they offer greater flexibility in the design and control of absorber
features and can be tailored to suit requirements. This article reviews various
classes of patterned structures: photonic crystals, metal–dielectric–metal slab
arrays, metamaterials, and nanostructures operating in the visible and infrared
wavelength ranges. Operation requirements, design principles and under-
lying physical phenomena, material and temperature considerations, as well
as fabrication methods are discussed. Recent progress in achieving various
desirable absorber features, such as broadband and multiband operation,
polarization and angle independence, flexibility, and tunability is presented.
Suggestions are also given regarding future research directions.
Dr. I. E. Khodasevych, Prof. A. Mitchell
School of Electrical and Computer Engineering
ARC Centre for Ultrahigh Bandwidth
Devices for Optical Systems (CUDOS)
RMIT University
GPO Box 2476, Melbourne, VIC 3001, Australia
E-mail: iryna.khodasevych@rmit.edu.au
Dr. L. Wang
School for Engineering of Matter
Transport and Energy
Arizona State University
Tempe, Arizona 85287, USA
Prof. G. Rosengarten
School of Aerospace
Mechanical and Manufacturing Engineering
RMIT University
GPO Box 2476, Melbourne, VIC 3001, Australia
satisfy world's current and future energy
demands.
[2]
Also, this supply is practi-
cally endless. Solar energy has been used
for heating and cooling of air and water
in domestic as well as industrial applica-
tions, electricity generation and chemical
reactions. However, there are challenges
toward efficiently extracting this energy
and converting it into other, usable forms.
One of the better-known means of
harnessing solar energy is photovoltaics
( Figure 1a), where solar radiation is con-
verted into electricity with the help of
various semiconducting materials, exhib-
iting the photovoltaic effect and referred
to as solar or photovoltaic cells.
[3–5]
Expo-
sure of the solar cell to light triggers the
generation of electron–hole pairs, car-
rying an electric current, thus the system
is dependent on the band structure of the
corresponding material. Only a narrow
spectral range of light waves with suitable
energies are used in the conversion process, while the majority
of the solar spectrum is left unutilized, resulting in a low
photon-to-electron conversion efficiency.
The light incident on a photovoltaic cell, however, is not
required to originate from the sun. In the field of thermo-
photovoltaics (TPV) (Figure 1b), a thermal emitter heated to a
high temperature serves as a source of radiation.
[6,7]
Emitters
are typically heated to temperatures in the range of thousands
of degrees Celsius, so that they emit most of the radiation in
the infrared, where the corresponding energy bands of semi-
conductors, used in photovoltaic cells, are located. Solar TPVs
(Figure 1c) use solar energy to heat the emitter and take advan-
tage of concentrators that focus the radiation collected over a
larger area onto a much smaller photovoltaic system, thus
reducing the material costs. Such systems allow the conversion
of energy stored in wide solar spectrum into the narrow range
of frequencies suitable for photovoltaic cell operation, thus
increasing the overall efficiency.
[8]
Solar thermal systems (Figure 1d) use solar radiation
to create heat, which can be used directly for applications
including industrial processes or absorption cooling.
[9]
Such
systems can also be harnessed for electricity generation through
the use of turbines. Ideally, solar thermal receivers will absorb
strongly in the visible and NIR regions to extract the optimal
energy from solar radiation, but will have suppressed emis-
sivity in the mid to far infrared so that, when the solar radiation
is converted into heat, this heat is trapped within the absorber
Adv. Optical Mater. 2015,
DOI: 10.1002/adom.201500063
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