High-performance planar solar concentrators based on nanoparticle doping
A light scattering-based solar concentrator (LSSC) uses high refractive index nanoparticles (NPs) as dopants to selectively scatter photons across the solar spectrum without spectroscopic conversion by different sized nanoparticles. The LSSCs are limited by a single parameter: the surface photon losses, which can be addressed by nanofabrication to implement anti-reflective and light trapping structures into LSSC designs. The LSSC design provides solar concentrator techniques for photovoltaic (PV) applications.
1. A light scattering-based solar concentrator (LSSC) for photovoltaic (PV) applications, comprising:
a plurality of solar cells;
dielectric oxide nanoparticles (NPs) having a refractive index greater than 2.0 dispersed in a binder formed as a waveguide attached to the plurality of solar cells,
wherein the NPs are confined to a central scattering layer sandwiched between non-scattering layers within the waveguide and said non-scattering layers do not contain NPs,
said LSSC having at least one layer of nanostructure combining anti-reflective and light trapping on a surface toward an inside of the waveguide to reduce photon surface loss, and
one or more reflectors are attached to one or more surfaces of the waveguide to reflect transmitted light,
wherein the LSSC has a device concentration ratio C>1 and a device power conversion efficiency (η SC ) from 5.26% to 7.58%, where C is the device concentration ratio, which is the ratio between output electrical power from the solar concentrator (P SC ) and the output electrical power of the solar cells (P cell ) under the same incident condition as defined by the following equation:
C
=
P
SC
P
cell
=
η
SC
A
SC
H
i
n
η
cell
A
cell
H
i
n
=
η
SC
η
cell
×
A
SC
A
cell
=
P
×
G
where G is device geometric gain and is defined as the ratio between A SC and A cell , where A SC is top surface area of the device and A cell is the area of the solar cells, P is device optical efficiency defined as the ratio between the device power conversion efficiency (η SC ) and the cell conversion efficiency (η cell ), and H in is the incident power density.
2. The LSSC according to claim 1 further comprising a luminescence solar concentrator (LSC) placed on top of the LSSC to form a hybrid structure.
3. The LSSC according to claim 1 wherein the NPs have a diameter in a range of 100 nm to 800 nm.
4. The LSSC according to claim 3 wherein the NPs have a diameter in a range of 250 nm to 500 nm.
5. The LSSC according to claim 1 wherein the NPs are uniformly dispersed in the binder.
6. The LSSC according to claim 1 wherein the binder includes one or more of polymethyl methacrylate (PMMA) or methyl methacrylate (MMA).
7. The LSSC according to claim 1 wherein the NPs are TiO 2 having diameter sizes ranging from 100 nm to 800 nm.
8. The LSSC according to claim 7 wherein the binder is at least one polymer selected from the group consisting of polymethylmethacrylate, polycarbonate, polydimethylsiloxane polymer, and peflourinated perfluorinated polymer.
9. The LSSC according to claim 7 further comprising one or more fluorescence particles dispersed in the binder.
10. The LSSC according to claim 1 further comprising one or more fluorescence particles dispersed in the binder.
11. The LSSC of claim 1 , wherein said non-scattering layers comprise at least one polymer selected from the group consisting of polymethylmethacrylate, polycarbonate, polydimethylsiloxane, and perfluorinated polymer.