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Electrical and thermal properties of the metastable defect in boron-doped Czochralski silicon (Cz-Si)

: Rein, S.; Rehrl, T.; Warta, W.; Glunz, S.W.; Willeke, G.

Volltext urn:nbn:de:0011-n-2097990 (244 KByte PDF)
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Erstellt am: 27.10.2012

McNelis, B. ; WIP - Renewable Energies, München:
17th European Photovoltaic Solar Energy Conference 2001. Vol.2 : Proceedings of the international conference held in Munich, Germany, 22 - 26, October 2001
München: WIP-Renewable Energies, 2002
ISBN: 3-936338-07-8
ISBN: 88-900442-3-3
European Photovoltaic Solar Energy Conference <17, 2001, München>
Konferenzbeitrag, Elektronische Publikation
Fraunhofer ISE ()

Lifetime degradation observed in boron-doped Czochralski silicon (Cz-Si) has its origin in a metastable defect that is activated under illumination or forward bias and deactivated under an anneal at around 200°C. To give insight into the physical mechanism underlying this defect transformation, the first part of this study is focused on the kinetics of defect formation and annihilation. For the process of defect formation, the quantitative analysis of this work clearly shows that it cannot be directly described by the mechanism of recombination-enhanced defect reaction (REDR) as it has been proposed in recent studies. While REDR predicts for the defect generation rate U(ind gen) a linear dependence on the doping concentration N(ind A) and the injection level delta n, a quadratic doping and a vanishing injection dependence is found by an improved time-resolved degradation experiment measured with quasisteady-state photoconductance technique. The experiment reveals that U(ind gen) reaches almost its maximum value if delta n only lies above some threshold value, which is already reached for an illumination with 1 mW/cm2 on a 0.86 omega cm Cz-sample. For the process of defect annihilation, an isothermal annealing experiment reveals that it is thermally activated with an energy barrier E(ind barr) = 1.32 ± 0.05 eV, determined for the first time. The last part of the study is dedicated to the electronic structure of the defect. From temperature-dependent lifetime spectroscopy (TDLS) an upper limit of 0.41 eV is found for the energy level of the Cz-defect in its active state. If the TDLS-result of this work is combined with the energy range determined by Schmidt et al. from injection dependent lifetime spectroscopy, the energy level of the defect in its active state can be further localized in the lower band half at E(ind V) + 0.35...0.41 eV.