Modeling characteristic curves of solar cells and optical detectors with the Simmon–Taylor approximation

• Amorphous and microcrystalline silicon based electronic devices.
• Charge trapping and recombination described by the Simmon–Taylor Approximation
• This approximation simplifies the Schockley–Read–Hall formalism.
• Characteristic curves evaluated at various illuminations, temperatures, voltages.
• The Aproximation is acceptable in solar cell modeling and in optical detectors.

The performance of amorphous and microcrystalline silicon based electronic devices is highly dependent on the density of states present in the band gap. The density of states in these materials contains two exponentially decreasing tails and a high number of deep states. Charge trapping and the recombination of electron–hole pairs through gap states are usually described by the Schockley–Read–Hall (SRH) formalism. The equations derived in the SRH formalism can be highly simplified by using the Simmons–Taylor's algorithms, especially the one so called “0 K” approximation, which allows a quasi-analytical derivation of the current–voltage characteristics. Although the validity of these algorithms were discussed in the literature on semiconductor materials, there is not a systematic study where these algorithms were included in a computer code that numerically solves the governing semiconductor device equations in order to compare the characteristic curves predicted by these simplifications with the ones obtained with the SRH formalism. This paper is an attempt to fill this void. The approximations of Simmon–Taylor were implemented in our code D-AMPS and the current–voltage and spectral response curves were evaluated under different conditions: with and without bias light, at forward and reverse bias voltages, at different temperatures, for various intrinsic layer thicknesses and for different key electrical parameters. To simplify the discussion we have assumed a uniform density of states along the intrinsic layer. Our results indicate that the Simmon–Taylor approximation is acceptable when the device is working under illumination. Under dark conditions the approximation is also satisfactory when the device is forward biased but slightly overestimates the dark current when the device is reverse forward. Although the 0 K approximation leads us to unacceptable results when the device is reversed biased and operates under dark conditions it can also be used in device modeling taking some precautions.