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Topologically Defined Neuronal Networks Controlled by Silicon Chips

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CHAPTER 2. NETWORKS OF DEFINED TOPOGRAPHY<br />

naptic spikes were only fired in neuron 1 upon presynaptic stimulation of 2. Neuron 2 was depolarized<br />

only a little when it was postsynaptic and remained quiescent.<br />

To localize the synapse in the network depicted in the bottom row of fig. 2.21, it was stained with<br />

Lucifer Yellow, first cell 1, see left micrograph, then cell 2, as shown in the right micrograph. Most<br />

neurites nicely followed the grooves, only a small one left the structure at the pit of neuron 1. Compared<br />

to example 2.19, the position of the synapse was much less defined here. The neurite from cell 2 grew<br />

in parallel to that of neuron 1. Note the white ‘dots’ in the left side groove in the left micrograph indicating<br />

the presence of a rather thin neurite originating from 1. The synapse must be somewhere along<br />

the line of fasciculated growth of both neurites marked in the right micrograph, but its exact location is<br />

unknown.<br />

Electrophysiological recordings revealed a very strong connection, the averaged coupling coefficients<br />

were k1,2=0.69 and k2,1=0.51. Most presynaptic APs in neuron 1 also triggered spikes in cell 2. Changing<br />

the direction of signal transfer resulted in even stronger postsynaptic activity, with every spike in 2<br />

triggering a spike in cell 1.<br />

Given the examples above, one might conclude that the strength of synaptic coupling is the only parameter<br />

governing the generation of postsynaptic action potentials, with a larger coupling coefficient<br />

increasing the probability for a spike being triggered. However, the resting membrane potential of the<br />

postsynaptic neuron plays an important role, as well. If it is very high, near the firing threshold, just a<br />

small increase of the membrane potential is sufficient to trigger an AP. In this case, even a weak synaptic<br />

coupling is sufficient. But if the resting potential is rather low, a large postsynaptic depolarization<br />

resulting from a strong synapse may still not be sufficient to raise the cell above its firing threshold.<br />

Therefore, two parameters have to be taken into account when discussing the triggering of postsynaptic<br />

action potentials, the coupling coefficient and the respective resting potential.<br />

2.5.4 Characterization of synapses<br />

Of 84 networks grown on SU-8 structures in this assay, 51 were synaptically connected, but only 26<br />

were evaluated in detail. The others had ambiguous connection patterns that made the assignment<br />

of coupling to an identified synapse impossible, e.g. three neurons with unknown signaling path. Fig.<br />

2.22A shows a histogram of coupling coefficients for the 26 pairs. Two values are included per pair, one<br />

for each direction of signal transfer k1,2 and k2,1. The numbers are averaged from several recordings<br />

with currents of different amplitude injected in the cell pair. Most values range between 0.1 and 0.6,<br />

with extrema of 0.01 and 0.78. In general, they are higher than the coupling coefficients in networks on<br />

UV-patterned substrates [79] and the example net depicted in fig. 2.20. Still, they are well within the<br />

range found with the mollusks Helisoma and Aplysia on plain, unpatterned substrates [7, 41].<br />

Although the coupling coefficient is an ideal quantity for describing the effects of the presynaptic input<br />

on a postsynaptic neuron, it conveys only limited information about the synapse itself. As shown <strong>by</strong><br />

eq. 2.24, kpre,post is not only determined <strong>by</strong> synaptic properties but also <strong>by</strong> the soma conductance<br />

of the postsynaptic neuron. The synaptic conductance Gsyn is the quantity that entirely characterizes<br />

electrical synapses. It is determined from electrophysiological recordings <strong>by</strong> the following procedure:<br />

36<br />

– First, VA,0 and VB,0 are obtained from recording the membrane potentials of both neurons, A and<br />

B, before current injection.<br />

– Then, a constant hyperpolarizing current Iinj,∞ is injected in neuron A and the stationary presynaptic<br />

and postsynaptic response is measured after initial transients have decayed, VA,∞ and VB,∞.<br />

GA, GB and V0B are calculated from 2.26, 2.27 and 2.28.<br />

– The steps above are repeated to determine V0A, but this time with B as the presynaptic neuron where

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