Abstract Generation–recombination noise modelling of semiconductor devices through the impedance field method customarily exploits, as microscopic noise sources, approximate equivalent current density fluctuations derived in a homogeneous system; moreover, such an equivalent approach often makes use of a monopolar (majority carrier) model only. Taking, as a reference model, an accurate numerical implementation of the Langevin approach wherein electron and hole density fluctuations are applied to a bipolar drift-diffusion physics-based model, we show that the approximate equivalent approach is inaccurate, even in a uniformly doped sample, unless the effect of the ohmic boundary conditions is negligible. Moreover, the monopolar equivalent model introduces further inaccuracies whenever minority carrier fluctuations are not negligible; this is shown to occur not only for direct processes, but also for trap-assisted transitions involving deep levels in a p - or n -doped semiconductor. The equivalent models are finally shown to match the exact approach only if the carrier lifetimes and fluctuation spectra are corrected empirically.
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