Bilateral processing in chemical synapses with electrical ‘ephaptic’ feedback: A theoretical model
Introduction
Classically, chemical synapses are polarized: they convey information from the presynaptic to the postsynaptic cell. However, retrograde signaling generated in the postsynaptic cell, either by chemical messengers [1], [2], [3] or by electric fields [4], [5], [6], may influence the functioning of the presynaptic neuron. Retrograde signaling created in the postsynaptic neuron by the electric field, may provide a very fast local activation (positive feedback, [5]) or inhibition (negative feedback, [7]). In the case of positive feedback, the current generated in the postsynaptic neuron would modify transmitter release by directly changing the presynaptic potential at the release site [4], [6], [8]. The ephaptic feedback should occur mainly in synapses with large synaptic contacts [9]. In accordance with these predictions, it was previously showed that hyperpolarising the postsynaptic neuron produces a supralinear increase in the amplitude of the mossy fiber (MF) EPSCs [5], [10]. The increase was stronger than that predicted from the shift in the driving force and was restricted only to large MF inputs to CA3 pyramidal cells (and not to the associative-commissural fiber synapses). Perhaps surprisingly, this supralinear increase was found to correlate with common indicators of the synaptic release probability [10]. However, the biophysical mechanism underlying these phenomena remained largely unexplained [5], in spite of the fact that the paired recording revealed the possible ephaptic connection in hippocampal mossy fiber boutons [11] and at the giant calyx of Held synapse [12]. In such recordings, the ephaptic signals have been seen as either a capacitative transient that precedes the postsynaptic current [12] or a relatively small ephaptic currents in a presynaptic neuron [11]. In addition, the capacitance-coupled activity in the postsynaptic neuron (antidromic ephaptic signal) shows up as a ‘postpotential’ following the falling phase of the presynaptic spike (see Fig. 4d in [13]).
In the present study, I propose a complex dynamic model of synaptic transmission, which includes the electrical ‘ephaptic’ feedback between postsynaptic and presynaptic membranes. Parameters and mechanisms used in the model correspond to what has been observed in the giant calyx of Held synapses where ephaptic effects should be particularly strong. The proposed model takes into account (i) the dynamics of calcium concentration in the presynaptic terminal, (ii) the kinetics of vesicle fusion, (iii) glutamate dynamics within the cleft, and (iv) activation of postsynaptic glutamate receptors. My findings extend the conclusions of previous theoretical calculations [14], suggesting that the ephaptic feedback can be sufficiently strong to modulate synaptic efficacy.
Section snippets
General description of the electrical processes in a chemical synapse
In the scheme of Fig. 1 the simulated synapse is represented. This consists of three parts, the axonal, the pre-, and the postsynaptic areas separated by the synaptic cleft.
The presynaptic part consists of two compartments. The first faces the extracellular space; the second is in front of the synaptic cleft. I shall refer to these two compartments as ‘extrasynaptic’ (or ‘out of the cleft’) and ‘intrasynaptic’ (or ‘cleft’), respectively. In the Calyx of Held the surface areas of extra- (S1) and
AP waveforms differ in the two presynaptic compartments
My model predicts that the presynaptic potentials V1 and V2 exert a direct electrical influence on the EPSC (4). The influence is stronger the greater is the difference between V1 and V2. This in turn depends on a number of parameters, the major one being the resistance of the synaptic cleft R. For example, if R is so small that can be neglected (R < 1 MΩ) the values of potentials are V1 = V2 and thus the set of the Eqs. (1), (2), (3), (4) takes the simplest form (A.7), (A.8), (A.9). In this case,
Discussion
The present study proposes the dynamic model of electrical feedback in chemical synapses. In contrast to previous stationary models [5], [10], [14], this model includes the dynamics of AP in the presynaptic terminal (including the underlying ionic and capacitative currents), detailed kinetics of calcium dynamics in the synaptic vicinity, vesicle fusion, glutamate diffusion within the cleft and activation of AMPA and NMDA receptors.
My simulations predict several important phenomena. First, the
Acknowledgments
I am grateful to Dr. Enrico Cherubini and Dr. Dmitri A. Rusakov for helpful discussions and critical reading of the manuscript. Also I thank the anonymous reviewer for his valuable comments on the manuscript.
I was a fellow of the ICTP Programme for Training and Research in Italian Laboratories, Trieste, Italy. The part of the work was supported by grants from INTAS program (No. 47, 2002–2005).
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