NUSOD '05. Proceedings of the 5th International Conference on Numerical Simulation of Optoelectronic Devices, 2005.
DOI: 10.1109/nusod.2005.1518128
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Injection dependence of spontaneous radiative recombination in c-Si: experiment, theoretical analysis, and simulation

Abstract: The radiative recombination coefficient B in crystalline bulk silicon is enhanced by the Coulomb attraction between electrons and holes. This effect -and hence B -is reduced at high carrier densities due to screening. We measure and numerically calculate B as a function of injection density, and with the gained model we simulate an experiment in order to extract the Coulomb-enhancement of Auger recombination.

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Cited by 30 publications
(18 citation statements)
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“…The bulk component τ b includes the intrinsic components due to Auger and radiative recombination , which will here be described by Richter's parameterisation , with the radiative recombination term B rel from Ref. and B low from Ref. .…”
Section: Characterising Surface Passivationmentioning
confidence: 99%
“…The bulk component τ b includes the intrinsic components due to Auger and radiative recombination , which will here be described by Richter's parameterisation , with the radiative recombination term B rel from Ref. and B low from Ref. .…”
Section: Characterising Surface Passivationmentioning
confidence: 99%
“…The equation for τ bulk as a function of excess carrier concentration (∆n) is: (6) In Equation 4, B low is the radiative recombination coefficient as measured by Trupke 15 for lightly doped silicon and B rel is the relative radiative recombination coefficient determined by Altermatt. 14 The product of these two coefficients account for the radiative recombination component of bulk crystalline silicon. Both B low and B rel are temperature sensitive.…”
Section: A Bulk Recombination Modelmentioning
confidence: 99%
“…The gray, solid lines show the variation of the dynamic PL lifetime due to the injection-dependent lifetime from numerical simulations, assuming that the photoconductance-based lifetime measurements represent the actual steady-state carrier lifetimes. Furthermore, we take the injection-dependent coefficient of radiative recombination into account that describes the decreasing probability of radiative recombination with increasing injection density [10]. The gray dashed lines are modeled by assuming a 10% uncertainty of the PC-based lifetime measurement [11].…”
Section: Dynamic Pl Lifetime Measurementsmentioning
confidence: 99%