2017
DOI: 10.1002/pssc.201600171
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Local structure analysis of Cu(In,Ga)Se2 by X‐ray fluorescence holography

Abstract: X‐ray Fluorescence Holography (XFH) study of Cu(In,Ga)Se2 single crystals has been performed using an inverse mode. Energies of incident X‐ray are from 9.2 to 13.2 keV. The Cu‐Kα X‐ray fluorescence hologram has been constructed, and atomic images were reconstructed using Barton's algorithm. Dependence of fluorescent X‐ray, either Cu or Ga, on the reconstructed atomic images of CuIn0.2Ga0.8Se2 was examined. The atomic image of CuIn0.2Ga0.8Se2 was compared with that of CuIn0.8Ga0.2Se2. The reconstructed atomic i… Show more

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“…The decline of accurate τ bulk determination for higher doping levels is a significant limitation because doping N A ≥ 10 14 cm −3 is needed in photovoltaic devices where minority charge carrier collection is aided by the junction field. Arsenic‐doped CdTe devices have reached doping levels of 10 15 –10 16 cm −3 , [ 20–22 ] Cu(In,Ga)Se 2 (CIGS) solar cell doping levels are typically 10 15 –10 16 cm −3 due to intrinsic defects, [ 23–27 ] and doping in perovskite solar cells can exceed 10 16 cm −3 . [ 28 ] Therefore, bulk recombination lifetime determination in doped absorbers is relevant for multiple PV technologies.…”
Section: Introductionmentioning
confidence: 99%
“…The decline of accurate τ bulk determination for higher doping levels is a significant limitation because doping N A ≥ 10 14 cm −3 is needed in photovoltaic devices where minority charge carrier collection is aided by the junction field. Arsenic‐doped CdTe devices have reached doping levels of 10 15 –10 16 cm −3 , [ 20–22 ] Cu(In,Ga)Se 2 (CIGS) solar cell doping levels are typically 10 15 –10 16 cm −3 due to intrinsic defects, [ 23–27 ] and doping in perovskite solar cells can exceed 10 16 cm −3 . [ 28 ] Therefore, bulk recombination lifetime determination in doped absorbers is relevant for multiple PV technologies.…”
Section: Introductionmentioning
confidence: 99%