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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Li, S. X.
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (5/5 displayed)
- 2009Properties of native point defects in In1-xAlxN alloyscitations
- 2006Multiband GaNAsP quaternary alloyscitations
- 2006Structure and electronic properties of InN and In-rich group III-nitride alloyscitations
- 2004Group III-nitride alloys as photovoltaic materialscitations
- 2003Band-gap bowing effects in BxGa1-xAs alloyscitations
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article
Group III-nitride alloys as photovoltaic materials
Abstract
The direct gap of the In<sub>1-x</sub>Ga<sub>x</sub>N alloy system extends continuously from InN (0.7 eV, in the near IR) to GaN (3.4 eV, in the mid-ultraviolet). This opens the intriguing possibility of using this single ternary alloy system in single or multi-junction (MJ) solar cells. A number of measurements of the intrinsic properties of InN and In-rich In <sub>1-x</sub>Ga<sub>x</sub>N alloys (0 <x <0.63) are presented and discussed here. To evaluate the suitability of In<sub>1-x</sub>Ga<sub>x</sub>N as a material for space applications, extensive radiation damage testing with electron, proton, and alpha particle radiation has been performed. Using the room temperature photoluminescence intensity as a indirect measure of minority carrier lifetime, it is shown that In<sub>1-x</sub>Ga<sub>x</sub>N retains its optoelectronic properties at radiation damage doses at least 2 orders of magnitude higher than the damage thresholds of the materials (GaAs and GaInP) currently used in high efficiency MJ cells. Results are evaluated in terms of the positions of the valence and conduction band edges with respect to the average energy level of broken-bond defects (Fermi level stabilization energy E<sub>FS</sub>). Measurements of the surface electron concentration as a function of x are also discussed in terms of the relative position of E <sub>FS</sub>. The main outstanding challenges in the photovoltaic applications of In<sub>1-x</sub>Ga<sub>x</sub>N alloys, which include developing methods to achieve p-type doping and improving the structural quality of heteroepitaxial films, are also discussed.