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This invention relates to structures and techniques for construction of solar cells based on III-V materials, such as gallium and arsenide. More particularly, this invention relates to the problem of forming reliable electrically conductive contacts for electrical terminals for devices or structures incorporating III-V materials.
Conventional or known III-V GaAs-based solar cells can be divided into three parts—a lower part, a middle part, and an upper part, as shown in cross-sectional representation in
Generally, the metal and semiconductor layers in the upper part 30 are patterned into a grid of lines 40 as shown in
The layer that faces the sun is referred to as the uppermost or top layer of the uppermost junction. Most solar cell junctions consist of a thin n-type emitter region on top of a thicker p-type base region (an “n-on-p” type structure). For the cell to work properly, all junctions within the III-V stack must have the same orientation. Thus, if one junction is an ‘n-on-p” type, all junctions in the cell must the same. Junctions within the multijunction solar cell stack may include back and front surface fields. Tunnel junctions may connect the various sub-cell p-n junctions.
Because of the need for a uniform orientation of the junctions within the III-V stack, a standard “n-on-p” type solar cell is typically grown on a p-doped substrate such as p-GaAs or p-Ge. The substrate in such cells often is used as the bottom layer of the lowermost junction. However, p-doped GaAs substrates are typically more expensive than the alternative n-type or semi-insulating (SI) varieties. It would be desirable, therefore, to reduce the production cost of “n-on-p” type solar cells by using a lower cost n-doped growth substrate. To do so directly, however, would create a reverse orientation of the lowermost junction, thus causing the solar cell to not operate properly.
According to the invention, a method is provided for using n-GaAs (or other n-doped semiconductor material) as the substrate for “n-on-p” type solar cell designs by depositing a “p-on-n”tunnel junction diode as the first layer of material above the substrate and depositing the entirety of the III-V stack above the tunnel diode. Other layers may be grown between the substrate and the first tunnel junction, provided the type of doping of the other layers is either n-type or undoped. This first tunnel junction, like the other tunnel junctions in the solar cell, operates in an electrically non-rectifying regime. Electrically, the tunnel junction operates like a low resistance resistor and does not block current flow.
The invention will be better understood by reference to the following detailed description in connection with the accompanying drawings.
A specific embodiment uses a dilute nitride sub-cell above the tunnel junction 50, rendering the solar cell capable of absorbing longer wavelength energies without having to rely on use of the substrate as part of the sub-cell structure. This embodiment is particularly advantageous as it combines long wavelength sub-cell capability with low cost n-type GaAs substrates, where all base and emitter layers in the solar cell are lattice matched to one another. A dilute nitride is generally considered to be a Type-III-V semiconductor alloy having less than 5% nitrogen content. The term longer wavelengths in this context refers to wavelengths corresponding to energies of less than 1.42 eV, which is equivalent to the bandgap of pure GaAs, or greater than approximately 870 nm wavelength. Lattice matched layers have a crystal structure which is coherent and does not relax or break down from layer to layer despite the possibility of strain in the layers.
The bandgap and lattice constant of a dilute nitride can be changed independently through proper choice of composition, allowing dilute nitrides, for example, to be lattice matched to Gallium Arsenide substrates, and have an optimal bandgap for a particular device design. For example, in the case of a triple junction solar cell, the optimal bandgap of the longest wavelength junction is around 1 eV (0.93 eV to 1.05 eV). Such a bandgap can be achieved using dilute nitride material while maintaining lattice match to GaAs. This type of triple junction solar cell may have a second junction and a third junction that are constructed of Gallium-Arsenide and Indium-Gallium-Phosphide. In this case, the bulk of all of the n-on-p junctions can be lattice matched to the substrate.
Another specific embodiment involves the use of a Silicon-Germanium alloy as the longest wavelength absorbing junction. Silicon-Germanium material can be readily lattice matched to a GaAs substrate. Lattice matching to GaAs is achieved through the addition of approximately 2% Silicon to Germanium. The Silicon is added to Germanium specifically to promote lattice matching of the sub-cell to a Gallium-Arsenide substrate. Such a material has a bandgap close to 0.7 eV. Triple junction devices comprising a Silicon-Germanium sub-cell can be constructed similarly to the above mentioned dilute nitride based structure.
An “n-on-p” type solar cell fabricated on an n-GaAs substrate utilizes this approach.
The invention will work with many different multijunction devices having from 1-to-n junctions (where n>1). Those skilled in the art will readily understand that solutions applicable to a two or three junction device will also be useful for more or fewer junctions, such as a four-junction solar cell or a five junction solar cell. The invention can be used with many different materials and configurations that are used to make solar cells and solar cell junctions, including without limitation dilute nitride materials, metamorphic InGaAs layers, quantum dots, quantum wells and the like. The invention described herein is applicable to any generalized “n-on-p” type solar cell device in which all solar absorbing junctions are contained within the stack 20 shown in
The invention has been explained with reference to specific embodiments. Other embodiments will be evident to those of skill in the art. It is therefore not intended that the invention be limited, except as indicated by the appended claims.
The present application claims benefit under 35 USC 119(e) of U.S. provisional Application No. 61/262,374, filed on Nov. 18, 2009, entitled “MULTIJUNCTION SOLAR CELLS FORMED ON N-DOPED SUBSTRATES,” the content of which is incorporated herein by reference in its entirety.
Number | Date | Country | |
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61262374 | Nov 2009 | US |