Details
Original language | English |
---|---|
Article number | 054508 |
Journal | Journal of Applied Physics |
Volume | 111 |
Issue number | 5 |
Publication status | Published - 8 Mar 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%.
ASJC Scopus subject areas
- Physics and Astronomy(all)
- General Physics and Astronomy
Cite this
- Standard
- Harvard
- Apa
- Vancouver
- BibTeX
- RIS
In: Journal of Applied Physics, Vol. 111, No. 5, 054508, 08.03.2012.
Research output: Contribution to journal › Article › Research › peer review
}
TY - JOUR
T1 - The effect of sample edge recombination on the averaged injection-dependent carrier lifetime in silicon
AU - Kessler, Michael
AU - Ohrdes, Tobias
AU - Altermatt, Pietro P.
AU - Brendel, Rolf
PY - 2012/3/8
Y1 - 2012/3/8
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%.
AB - 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%.
UR - http://www.scopus.com/inward/record.url?scp=84858975993&partnerID=8YFLogxK
U2 - 10.1063/1.3691230
DO - 10.1063/1.3691230
M3 - Article
AN - SCOPUS:84858975993
VL - 111
JO - Journal of Applied Physics
JF - Journal of Applied Physics
SN - 0021-8979
IS - 5
M1 - 054508
ER -