DS_Gabor_One
MEO_Gabor
ME_Gabor
MEO_Gabor_Rot
ME_Gabor_Rot
RD_Exp_T
Variations
MEO_Gabor.sHtQ
MEO_Gabor.sHtH
MEO_Gabor.sHt1
MEO_Gabor.sHt2
MEO_Gabor.s1tQ
MEO_Gabor.s1tH
MEO_Gabor
MEO_Gabor.s1t2
MEO_Gabor.s2tQ
MEO_Gabor.s2tH
MEO_Gabor.s2t1
MEO_Gabor.s2t2
This opponent motion energy (ME) model is perhaps the most idealized model of cortical direction selectivity. It was introduced by Adelson and Bergen (1985) and differs from their physiologically plausible ME model because its linear filters are 3-D Gabor functions (Gaussian times sinusoid). This model belongs to the class known as elaborated Reichardt detectors (van Santen and Sperling, 1984; Adelson and Bergen, 1985; van Santen and Sperling, 1985). Essentially, the model consists of the difference between the outputs (before spike generation) of two ME_Gabor (i.e., non-opponent) models that have opposite preferred directions. Like the ME_Gabor model, it provides an inadequate account of typical DS cells in macaque V1 and V5/MT (e.g., Bair and Movshon, 2004).
Results
References

The opponent signal (meopp) is then offset, scaled and half-wave rectified, and it is used to drive a Poisson spiking mechanism. The spikes are time shifted to simulate a neurobiological latency. See the model (.moo) files for the parameters that govern these computations.