The Jamming Avoidance Response inEigenmannia revisited: The structure of a neuronal democracy
To elicit JARs, S1 need not be phaselocked to the pacemaker. The JAR can thus be driven exclusively by electroreceptive afference, without reference to the pacemaker.
S1 and S2 may be pure sinewaves as long as their field geometries differ sufficiently. Higher harmonics, which may be added to a sinewave to mimic the EOD wave shape, are required only if S1 and S2 have identical geometries, i.e., if they are presented through the same pair of electrodes. The animal may thus use two different strategies to determine the sign of theδf: one which is based on differences in stimulus field geometries and one which is based on the presence of higher harmonics. Only the former is considered in the following.
The S1, but not the S2, field geometry should approximate the natural EOD field geometry. To the extent that this condition is violated, sufficiently high S2 intensities may elicit Anti-JARs (Fig. 4).
Evidence is given that the JAR is controlled, in a cumulative manner, by local interactions of neighboring electroreceptive fields on the animal's body surface which, as a consequence of different S1 and S2 field geometries, experience different degrees of contamination of S1 by S2. Simultaneous stimulations of remote areas of body surface result in almost linear summation of their associated effects on the pacemaker (Figs. 5, 6). Theoretically, no unitary central EOD representation is required.
Based on the results in 3. und 4., we propose that correct JARs are elicited to the extent that the majority of electroreceptors is predominantly driven by Sl rather than by S2, and this condition is fulfilled to the extent that the S1 field geometry approximates that of the natural EOD.
Effective S2 stimuli have a periodicity near that of the EOD (S1) fundamental frequency, f. This includes all stimuli with a power peak at a frequency of n·f+δf, n=l,2,3,t (Fig. 2), with the optimalδf being 3 to 8 Hz and identical for all n. Such stimuli cause consistent distortions in successive EODs (S1 pulses), which gradually travel through the EOD (S1) cycle (Fig. 3). This “motion” leads to periodic fluctuations in the amplitude of the joint signal, EOD (S1)+S2, and the phase of its positive zero-crossings with regard to those of the EOD (S1 (Fig. 7). The modulation of these two variables can be represented by a motion along a closed graph in a two-dimensional state plane (Fig. 8), which is reproducedδf times per s. The direction of motion along this graph reflects the sign of theδf. Evidence is given that this motion is detected by a mechanism comparable to a motion detector in the realm of vision.