Space radiation effects in InP solar cells

InP solar cells and mesa diodes grown by metalorganic chemical vapor deposition (MOCVD) were irradiated with electrons and protons at room temperature. The radiation-induced defects (RIDs) were characterized by deep level transient spectroscopy (DLTS), and the degradation of the solar cell performance was determined through I-V measurements. The nonionizing energy loss (NIEL) of electrons and protons in InP was calculated as a function of energy from 1 to 200 MeV and compared to the measured defect introduction rates. A linear dependence was evident. InP solar cells showed significantly more radiation resistance than c-Si or GaAs/Ge cells under 1 MeV electron irradiation. Using the calculated InP damage rates and measured damage factors, the performance of InP solar cells as a function of orbital altitude and time in orbit was predicted and compared with the performance of c-Si solar cells in the same environment. In all cases, the InP cells showed highly superior radiation resistance. >

[1]  P. W. Marshall,et al.  Correlation of Particle-Induced Displacement Damage in Silicon , 1987, IEEE Transactions on Nuclear Science.

[2]  J. Corbett Electron Radiation Damage in Semiconductors and Metals. , 1966 .

[3]  Cheryl J. Dale,et al.  Displacement damage in GaAs structures , 1988 .

[4]  R. Zuleeg,et al.  Energy Dependence of Proton-Induced Displacement Damage in Gallium Arsenide , 1987, IEEE Transactions on Nuclear Science.

[5]  Bourgoin,et al.  Threshold energy for atomic displacement in InP. , 1976, Physical review. B, Condensed matter.

[6]  M. Yamaguchi,et al.  First space flight of InP solar cells , 1990, IEEE Conference on Photovoltaic Specialists.

[7]  S. McKeever,et al.  Deep level transient spectroscopy of irradiated p‐type InP grown by metalorganic chemical vapor deposition , 1991 .

[8]  M. Yamaguchi,et al.  Injection-enhanced annealing of InP solar-cell radiation damage , 1985 .

[9]  Akio Yamamoto,et al.  High conversion efficiency and high radiation resistance InP homojunction solar cells , 1984 .

[10]  J. Bourgoin,et al.  Electron irradiation induced deep levels in p‐InP , 1982 .

[11]  R. Walters,et al.  Deep level transient spectroscopy study of proton irradiated p‐type InP , 1991 .

[12]  Edward A. Burke,et al.  Energy Dependence of Proton-Induced Displacement Damage in Silicon , 1986, IEEE Transactions on Nuclear Science.

[13]  M. Yamaguchi,et al.  Effects of impurities on radiation damage in InP , 1986 .

[14]  J. R. Carter,et al.  Solar cell radiation handbook , 1989 .

[15]  E. A. Wolicki,et al.  High energy electron induced displacement damage in silicon , 1988 .

[16]  M. Nastasi,et al.  Effect of particle-induced displacements on the critical temperature of YBa2Cu3O7−δ , 1989 .

[17]  C. J. Keavney,et al.  Emitter structures in MOCVD InP solar cells , 1990, IEEE Conference on Photovoltaic Specialists.

[18]  Masafumi Yamaguchi,et al.  Mechanism for radiation resistance of InP solar cells , 1988 .

[19]  Bruce E. Anspaugh,et al.  Solar cell radiation handbook. Addendum 1: 1982-1988 , 1989 .

[20]  M. Yamaguchi,et al.  Room‐temperature annealing of radiation‐induced defects in InP solar cells , 1984 .

[21]  J. Barengoltz,et al.  Correlation of Displacement Effects Produced by Electrons Protons and Neutrons in Silicon , 1975, IEEE Transactions on Nuclear Science.

[22]  Yamaguchi,et al.  Nonradiative-recombination-enhanced defect-structure trans- formation in low-temperature gamma -ray-irradiated InP. , 1986, Physical Review B (Condensed Matter).