Passive radiative
cooling is a method to dissipate excess heat
from a material by the spontaneous emission of infrared thermal radiation.
For a solar cell, the challenge is to enhance PRC while retaining
transparency for sunlight above the bandgap. Here, we design a hexagonal
array of cylinders etched into the top surface of silica solar module
glass to enhance passive radiative cooling. Multipolar Mie-like resonances
in the cylinders are shown to cause antireflection effects in the
infrared, which results in enhanced infrared emissivity. Using Fourier
transform infrared spectrometry we measure the hemispherical reflectance
of the fabricated structures and find the emissivity of the silica
cylinder array in good correspondence with the simulated results.
The microcylinder array increases the average emissivity between λ
= 7.5–16 μm from 84.3% to 97.7%, without reducing visible
light transmission.
The luminescent solar concentrator
(LSC) offers a potential pathway
for achieving low-cost, fixed-tilt light concentration. Despite decades
of research, conversion efficiency for LSC modules has fallen far
short of that achievable by geometric concentrators. However, recent
advances in anisotropically emitting nanophotonic structures could
enable a significant step forward in efficiency. Here, we employ Monte
Carlo ray-trace modeling to evaluate the conversion efficiency for
anisotropic luminophore emission as a function of photoluminescence
quantum yield, waveguide concentration, and geometric gain. By spanning
the full LSC parameter space, we define a roadmap toward high conversion
efficiency. An analytical function is derived for the dark radiative
current of an LSC to calculate the conversion efficiency from the
ray-tracing results. We show that luminescent concentrator conversion
efficiency can be increased from the current record value of 7.1–9.6%
by incorporating anisotropy. We provide design parameters for optimized
luminescent solar concentrators with practical geometrical gains of
10. Using luminophores with strongly anisotropic emission and high
(99%) quantum yield, we conclude that conversion efficiencies beyond
28% are achievable. This analysis reveals that for high LSC performance,
waveguide losses are as important as the luminophore quantum yield.
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