The present paper studies the issue of forming a diffraction concentrator in the form of relief diffraction gratings. The possibility of their application for solar energy systems based on GaAs heterostructures has been studied. It was shown that the use of diffractive and holographic concentrators proves to be very effective, since they provide for the increased radiant flux onto sensitive surface of the solar cell, whereas no automatic solar tracker is required. This will create novel approaches for a wide range application of gallium arsenide solar cells.
It is widely known, that solar cells are currently well developed on the basis of polycrystalline and single-crystal silicon. The highest possible efficiency ratio in laboratory samples is approximately 25% - 26%, and in commercially available solar cells developed on single crystals it reaches 20% - 22% and 16% - 18% for polycrystalline. The dimensions of the sensitive surface are 156 × 156 mm and the thickness is about 200 microns. The
share of silicon solar cells in the mass production is about 90%, whereas the share of thin-film solar cells in the world market is about 10%. Moreover, we are witnessing over the past few years certain achievements in the development of solar cells based on the cadmium telluride with an efficiency ratio of 20.4% for single trial samples, and 21.2% for solar cells based on thin-film cells of copper selenide-indium-gallium. Record efficiency was reported for the cascade solar cells based on compounds AIIIBIV, with ~44% efficiency ratio for the concentrated-solar-radiation types and 38.8% ratio for conventional types. However, in spite of these recent achievements in the development of solar cells it becomes necessary to compete with conventional energy based on hydrocarbons. This goal becomes achievable if we take into account the fact that 1 kW∙h of electricity generated by solar panels cost in 2008 approximately $US 0.35. Nowadays, this figure is already averages $US 0.11 - 0.12. The aim is to reduce the cost of 1 kW∙h to $ 0.08 - 0.09. In view of the above mentioned, the problem continues to be associated with the need to develop new designs and technologies to build solar cell structures effectively operating on the basis of novel scientific approaches, ideas and mechanisms. Therefore, the worldwide scientific community is in a constant search for new physical, technical and technological techniques, which could let obtain high efficiency solar cells. One solution to this problem is the development of novel physical foundations improving the efficiency of direct conversion of solar radiation into electrical energy using the recent achievements of modern nanotechnology (Nanophysics), holographic coatings, superlattices, functional ceramic layers, zero-dimensional inclusions. This will certainly contribute to the formation of novel technical, technological and design solutions for a new generation of solar cells.
In order to obtain high-performance, high-current semiconductor solar cells that directly convert solar radiation to electricity, it is necessary to develop the sandwich structures with varying band gap. Such multilayer (cascade) solar cells are currently being widely developed utilizing heterostructures based on Gallium Arsenide Aluminum Gallium Arsenide [
Gallium Arsenide heterostructure solar cells represent structures containing several epitaxial layers of GaInP, GaInAs or AlGaInP grown on a substrate of a single Germanium crystal. Implementation of such type of multi- cascade solar cells serves as a basis for generation of electron-hole pairs due to the absorption of wide spectral range of solar radiation. Such multi-cascade elements manifest stunning efficiency ratios (~40%) [
Hybrid holographic solar concentrator has the following design. Rectangular planes of holographic film
(
Hybrid holographic solar concentrator operates in the following manner. Solar radiation of various wavelengths runs through the upper plate 1 and then the layer 2 of the dye in the immersion liquid. Dye partially re-emits shorter wavelengths into the spectral region of absorption of the solar cells. When sunlight falls on the holographic grating, decomposed spectrum appears as a result of Bragg diffraction [
(d—the period of the holographic grating, θ—angle of diffraction)
Holographic grating parameters are chosen so as to meet the following two requirements. Firstly, the light with a wavelength λ1 equals the intrinsic absorption band of the material of the solar cell 5. Secondly, holographic gratings are oriented in such a manner that the angle of reflection (diffraction) of light with a wavelength λ1 for plate 1 be the total internal reflection angle. This leads to the event that radiation of this wavelength is reflected from the substrate-air interface and hits back the holographic grating, thus the process is repeated multiple times until the radiation is released through the central region free of holographic grating, passes through the second transparent plate 4 and falls onto solar cell 5.
A holographic planar concentrator [
The device described by V. A. Pilipovich [
The present paper describes the possibility of implementation of diffraction, holographic and spectral concentrators for solar concentration on solar cell based on GaAs heterostructures.
We have studied characteristics and properties of diffraction concentrators in the form of relief diffraction gratings with a frequency of bars of 40 mm — 1 made out of polyvinyl rectangular plates of 0.2 mm thickness with an area of 10 × 10 mm with bars of parallel faces. The plate was placed at a distance of 10 mm from the surface of cell and illuminated by remote light source. When illuminated, a strip with width of 10 mm of increased brightness appears beyond the area of shadow perpendicular to the plate. Measurements showed that the lighting (flux) in the area of increased brightness increases twofold and three-fold compared to normal brightness of the illuminated area. Thereafter, we measured the angles of illumination where the lighting in the area of increased brightness remains increased by 2 times. Measurements showed that the angle of lighting in the plane parallel to the grating grooves can vary in the range ±40˚, whereas in the plane perpendicular to the grating plane in the range ±30˚.
Based on these results we have trial tested the diffraction concentrator (
Illumination of solar cell does not change when lighting angles are ±40˚. The main advantage of the diffraction concentrator is ease of manufacture and low cost.
A holographic concentrator is also based on the use of reflective diffraction micro gratings obtained by holographic technique and embossed on polistrol film with reflective coating. Geometry of the micro gratings is calculated based on the main task of the holographic concentrator, i.e. to collect maximum solar radiation coming at different angles on GaAs solar cell panel (at daily movement of the sun). Based on the calculated geometry of
location of micro gratings and in accordance with technology of production of rainbow holograms [
Between glass plates 1 and 2 the immersion liquid 4 and holographic film 3 are inserted. Upon illumination of the cell by incident light 6 falling at different angles, variation of illumination on the light detector 5 was measured. Changing illumination angle within the range ±45˚ the illumination was steady increased 4 to 5 times.
Based on the results of trials we have been able to design hybrid solar concentrator [
Utilization of diffraction and holographic concentrators in the structure thus can increase the efficiency of use of solar radiation due to several factors:
· absence of the Sun tracking system;
· increased use of solar radiation while the total area of solar cell remains unchanged due to implementation of the organic dye for converting the short-wave part of the spectrum of solar radiation into radiation with a wavelength falling within the absorption band of the solar cell;
· reduced cost of solar panels due to reduced size of gallium arsenide solar cells.
All these serve as the basis for a wide scale application of gallium-arsenide solar cells.