The effect of sample edge recombination on the averaged injection-dependent carrier lifetime in silicon

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Autoren

  • Michael Kessler
  • Tobias Ohrdes
  • Pietro P. Altermatt
  • Rolf Brendel

Organisationseinheiten

Externe Organisationen

  • Institut für Solarenergieforschung GmbH (ISFH)
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Details

OriginalspracheEnglisch
Aufsatznummer054508
FachzeitschriftJournal of Applied Physics
Jahrgang111
Ausgabenummer5
PublikationsstatusVeröffentlicht - 8 März 2012

Abstract

In semiconductors, the effective excess carrier lifetime, τ eff, measured in dependence on the injection density, n, is an important parameter. It is frequently observed that τ eff decreases with decreasing n at low-level injection conditions (where Δn is smaller than the dopant density N dop), which has been difficult to explain. We compare measurements with numerical device simulations to demonstrate that this observed reduction of τ eff is caused by a combination of (i) Shockley-Read-Hall (SRH) recombination at the edges of the sample and (ii) transport effects of the carriers toward the edges. We measure τ eff(Δn) of boron-diffused and surface-passivated p +np ++ and p +pp ++ silicon wafers with the commonly applied photo-conductance decay technique, and we vary the sample size. The photo-conductance is probed by inductive coupling within a sample region of about 3 × 3 cm 2; hence, the measurements yield an average value of both τ eff,av and Δn av within that region. For a detailed analysis, we determine τ eff with a high spatial resolution using the dynamic infrared lifetime mapping technique, which shows a strong decrease of τ eff toward the edges of the p np samples at low-level injection. We analyze the measurements by numerical device modeling and circuit simulation. We conclude that the sample size should be at least 6 6 cm 2 for reliable τ eff(n) measurements at low injection conditions. However, at high-injection conditions, the recombination usually dominates at the dopant-diffused surfaces. Therefore, the saturation current-density, J 0, can be extracted from the τ eff(Δn) measurements in samples as small as 3 × 3 cm 2, with a measurement error due to edge recombination below 10%.

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The effect of sample edge recombination on the averaged injection-dependent carrier lifetime in silicon. / Kessler, Michael; Ohrdes, Tobias; Altermatt, Pietro P. et al.
in: Journal of Applied Physics, Jahrgang 111, Nr. 5, 054508, 08.03.2012.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Kessler M, Ohrdes T, Altermatt PP, Brendel R. The effect of sample edge recombination on the averaged injection-dependent carrier lifetime in silicon. Journal of Applied Physics. 2012 Mär 8;111(5):054508. doi: 10.1063/1.3691230
Kessler, Michael ; Ohrdes, Tobias ; Altermatt, Pietro P. et al. / The effect of sample edge recombination on the averaged injection-dependent carrier lifetime in silicon. in: Journal of Applied Physics. 2012 ; Jahrgang 111, Nr. 5.
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AU - Altermatt, Pietro P.

AU - Brendel, Rolf

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N2 - In semiconductors, the effective excess carrier lifetime, τ eff, measured in dependence on the injection density, n, is an important parameter. It is frequently observed that τ eff decreases with decreasing n at low-level injection conditions (where Δn is smaller than the dopant density N dop), which has been difficult to explain. We compare measurements with numerical device simulations to demonstrate that this observed reduction of τ eff is caused by a combination of (i) Shockley-Read-Hall (SRH) recombination at the edges of the sample and (ii) transport effects of the carriers toward the edges. We measure τ eff(Δn) of boron-diffused and surface-passivated p +np ++ and p +pp ++ silicon wafers with the commonly applied photo-conductance decay technique, and we vary the sample size. The photo-conductance is probed by inductive coupling within a sample region of about 3 × 3 cm 2; hence, the measurements yield an average value of both τ eff,av and Δn av within that region. For a detailed analysis, we determine τ eff with a high spatial resolution using the dynamic infrared lifetime mapping technique, which shows a strong decrease of τ eff toward the edges of the p np samples at low-level injection. We analyze the measurements by numerical device modeling and circuit simulation. We conclude that the sample size should be at least 6 6 cm 2 for reliable τ eff(n) measurements at low injection conditions. However, at high-injection conditions, the recombination usually dominates at the dopant-diffused surfaces. Therefore, the saturation current-density, J 0, can be extracted from the τ eff(Δn) measurements in samples as small as 3 × 3 cm 2, with a measurement error due to edge recombination below 10%.

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