A multijunction solar cell including a metamorphic layer, and particularly the design and specification of the composition, lattice constant, and band gaps of various layers above the metamorphic layer in order to achieve reduction in “bowing” of the semiconductor wafer caused by the lattice mismatch of layers associated with the metamorphic layer.

A multijunction solar cell including a metamorphic layer, and particularly the design and specification of the composition, lattice constant, and band gaps of various layers above the metamorphic layer in order to achieve reduction in “bowing” of the semiconductor wafer caused by the lattice mismatch of layers associated with the metamorphic layer.

Shockley-Read-Hall (SRH) generation and/or recombination in heterojunction devices is suppressed by unconventional doping at or near the heterointerface. The effect of this doping is to shift SRH generation and/or recombination preferentially into the wider band gap material of the heterojunction. This reduces total SRH generation and/or recombination in the device by decreasing the intrinsic carrier concentration n.sub.i at locations where most of the SRH generation and/or recombination occurs.

The physical basis for this effect is that the SRH generation and/or recombination rate tends to decrease as n.sub.i around the depletion region decreases, so decreasing the effective n.sub.i in this manner is a way to decrease SRH recombination.

A method for producing a mosaic solar cell assembly, comprising the steps of singulating a III-V compound semiconductor solar cell wafer into four identical discrete solar cell mosaic elements each substantially shaped as a quadrant of a circle, comprising a first and second solar cell mosaic element having one curved edge in the shape of an arc of the circumference of the circular wafer from which the element was singulated, and a single straight edge, rearranging and positioning two of the mosaic elements into a substantially rectangular mosaic assembly; providing a metal interconnect between each of the mosaic elements along one edge of the assembly so that the mosaic elements may be electrically connected to an adjacent mosaic assembly; and optionally bonding the cover glass support to the top of the mosaic assembly.

A method for producing a mosaic solar cell assembly, comprising the steps of singulating a III-V compound semiconductor solar cell wafer into four identical discrete solar cell mosaic elements each substantially shaped as a quadrant of a circle, comprising a first and second solar cell mosaic element having one curved edge in the shape of an arc of the circumference of the circular wafer from which the element was singulated, and a single straight edge, rearranging and positioning two of the mosaic elements into a substantially rectangular mosaic assembly; providing a metal interconnect between each of the mosaic elements along one edge of the assembly so that the mosaic elements may be electrically connected to an adjacent mosaic assembly; and optionally bonding the cover glass support to the top of the mosaic assembly.

Embodiments of the invention generally relate to photovoltaic devices. In one embodiment, a method for forming a gallium arsenide based photovoltaic device includes providing a semiconductor structure, the structure including an absorber layer comprising gallium arsenide. A bypass function is provided in a p-n junction of the semiconductor structure, where under reverse-bias conditions the p-n junction breaks down in a controlled manner by a Zener breakdown effect.

Embodiments of the invention generally relate to photovoltaic devices. In one embodiment, a method for forming a gallium arsenide based photovoltaic device includes providing a semiconductor structure, the structure including an absorber layer comprising gallium arsenide. A bypass function is provided in a p-n junction of the semiconductor structure, where under reverse-bias conditions the p-n junction breaks down in a controlled manner by a Zener breakdown effect.

In this photoelectric conversion element wherein group III-IV compound semiconductor single crystals containing zinc as an impurity are used as a substrate, the substrate is increased in size without lowering conversion efficiency. A heat-resistant crucible is filled with raw material and a sealant, and the raw material and sealant are heated, thereby melting the raw material into a melt, softening the encapsulant, and covering the melt from the top with the encapsulant. The temperature inside the crucible is controlled such that the temperature of the top of the encapsulant relative to the bottom of the encapsulant becomes higher in a range that not equal or exceed the temperature of bottom of the encapsulant, and seed crystal is dipped in the melt and pulled upward with respect to the melt, thereby growing single crystals from the seed crystal. Thus, a large compound semiconductor wafer that is at least two inches in diameter and has a low dislocation density of 5,000 cm.sup.−2 can be obtained, despite having a low average zinc concentration of 5×10.sup.17 cm.sup.−3 to 3×10.sup.18 cm.sup.−3, at which a crystal hardening effect does not manifest.

In this photoelectric conversion element wherein group III-IV compound semiconductor single crystals containing zinc as an impurity are used as a substrate, the substrate is increased in size without lowering conversion efficiency. A heat-resistant crucible is filled with raw material and a sealant, and the raw material and sealant are heated, thereby melting the raw material into a melt, softening the encapsulant, and covering the melt from the top with the encapsulant. The temperature inside the crucible is controlled such that the temperature of the top of the encapsulant relative to the bottom of the encapsulant becomes higher in a range that not equal or exceed the temperature of bottom of the encapsulant, and seed crystal is dipped in the melt and pulled upward with respect to the melt, thereby growing single crystals from the seed crystal. Thus, a large compound semiconductor wafer that is at least two inches in diameter and has a low dislocation density of 5,000 cm.sup.−2 can be obtained, despite having a low average zinc concentration of 5×10.sup.17 cm.sup.−3 to 3×10.sup.18 cm.sup.−3, at which a crystal hardening effect does not manifest.

Distributed Bragg reflectors are incorporated into the compositionally graded buffers of metamorphic solar cells, adding functionality to the buffer without adding cost. The reflection aids in collection in subcells that are optically thin due to low diffusion length, high bulk recombination, radiation hardness, partially-absorbing quantum structures, or simply for cost savings. Performance enhancements are demonstrated in GaAs subcells with QWs, which is beneficial when GaAs is not the ideal bandgap.