• Journal of Semiconductors
  • Vol. 41, Issue 3, 032701 (2020)
M. Benaicha1, L. Dehimi1、2, F. Pezzimenti3, and F. Bouzid4
Author Affiliations
  • 1Laboratory of Metallic and Semiconductor Materials, University of Biskra, Biskra 07000, Algeria
  • 2Faculty of Science, University of Batna, Batna 05000, Algeria
  • 3DIIES - Mediterranea University of Reggio Calabria, Reggio Calabria 89122, Italy
  • 4UDCMA - Research Center in Industrial Technologies, Algiers 16014, Algeria
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    DOI: 10.1088/1674-4926/41/3/032701 Cite this Article
    M. Benaicha, L. Dehimi, F. Pezzimenti, F. Bouzid. Simulation analysis of a high efficiency GaInP/Si multijunction solar cell[J]. Journal of Semiconductors, 2020, 41(3): 032701 Copy Citation Text show less

    Abstract

    The solar power conversion efficiency of a gallium indium phosphide (GaInP)/silicon (Si) tandem solar cell has been investigated by means of a physical device simulator considering both mechanically stacked and monolithic structures. In particular, to interconnect the bottom and top sub-cells of the monolithic tandem, a gallium arsenide (GaAs)-based tunnel-junction, i.e. GaAs(n+)/GaAs(p+), which assures a low electrical resistance and an optically low-loss connection, has been considered. The J–V characteristics of the single junction cells, monolithic tandem, and mechanically stacked structure have been calculated extracting the main photovoltaic parameters. An analysis of the tunnel-junction behaviour has been also developed. The mechanically stacked cell achieves an efficiency of 24.27% whereas the monolithic tandem reaches an efficiency of 31.11% under AM1.5 spectral conditions. External quantum efficiency simulations have evaluated the useful wavelength range. The results and discussion could be helpful in designing high efficiency monolithic multijunction GaInP/Si solar cells involving a thin GaAs(n+)/GaAs(p+) tunnel junction.
    ${\alpha _{{\rm{Si}}}} = - 0.425{\left( {E - {E_{\rm{g}}}} \right)^3} + 0.757{\left( {E - {E_{\rm{g}}}} \right)^2}-0.0224\left( {E - {E_{\rm{g}}}} \right),$ (1)

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    ${\alpha _{{\rm{Si}}}} = 0.0287{\rm{exp}}\left[ {2.72\left( {E - {E_{\rm{g}}}} \right)} \right],$ (2)

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    $J\left( E \right) = \frac{{qkT{{{m}}^*}}}{{2{\pi ^2}{\hbar ^3}}}T\left( E \right){\rm{ln}}\left( {\frac{{1 + {\rm{exp}}\left( {{E_{{\rm{FL}}}} - E} \right)/kT}}{{1 + {\rm{exp}}\left( {{E_{{\rm{FR}}}} - E} \right)/kT}}} \right)\Delta E,$ (3)

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    $T\left( E \right) \simeq {\rm{exp}}\left[ { - 2\int\limits_{ - {x_1}}^{{x_2}} {\left| {k\left( x \right)} \right|{\rm{d}}x} } \right].$ (4)

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    M. Benaicha, L. Dehimi, F. Pezzimenti, F. Bouzid. Simulation analysis of a high efficiency GaInP/Si multijunction solar cell[J]. Journal of Semiconductors, 2020, 41(3): 032701
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