By George L. Gerstein (auth.), Frank H. Eeckman (eds.)

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Brookhart and V. B. Mountcastle), Vol. 'l, Chap. 3, pp. 39-97. Am. Physiol. , Bethesda, Maryland. [21] Rinzel, J. (1985). Bursting oscillations in an excitable membrane model. In "Ordinary and Partial Differential Equatons", (ed B. D. Sleeman and R. J. Jarvis), pp. 304-316. Springer-Verlag, New York. [22] Rinzel, J. (1987). A formal classification of bursting mechanisms in excitable systems. In "Mathematical Topics in Population Biology, Morphogenesis, and Neurosciences," Lecture Notes in Biomathematics 71, (ed E.

And Vis. Sci. Supp.. 28 (1987) 197. S. , In vivo pathway tracing in rat visual cortex using potential sensitive dyes, in preparation. S. and Virga, A Organization of individual cortical axons projecting from area VI (area 17) to V2 (area 18) in the macaque monkey, Vis. • 4 (1990) 11-28. V. N. Optical recording of neuronal activity in an invertebrate central nervous system: simultaneous monitoring of several neurons. J. Neurophysiol.. 40 (1977) 1281-1291. , Changes in fluorescence, turbidity, and birefringence associated with nerve excitation, Proc.

Parameters as for Fig.!. 36 While it is still challenging our intuition to understand this period extension phenomenon biophysically, we have developed some mathematical insight by considering a simpler problem, synchronization of two identical cells coupled by gap junctions. Here we also found that for small values of gc burst duration was increased. Moreover, underlying this extension is the fact that although the two cells burst simultaneously the spikes alternate during the active phase. We discovered the reason for this out-of-phase spiking by again using techniques as described above which exploit time scale differences.

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Analysis and Modeling of Neural Systems by George L. Gerstein (auth.), Frank H. Eeckman (eds.)
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