A pair of integrate-and-fire model neurons driven by partially shared and correlated presynaptic events.
A Each of the neurons  and  receives input from  sources, of which  are excitatory and  are inhibitory. Both neurons share a fraction  of their excitatory and inhibitory sources, whereas the fraction  is independent for each neuron. Schematically represented spike trains on the left of the diagram show the excitatory part of the input; the inhibitory input is only indicated. A single source emits spike events with a firing rate , with marginal Poisson statistics. Correlated spiking is introduced in the  common excitatory sources to both neurons. This pairwise correlation is realized by means of a multiple interaction process (MIP) [39] that yields a correlation coefficient of  between any pairs of sources. In absence of a threshold, the summed input drives the membrane potential to a particular working point described by its mean  and standard deviation  and the correlation coefficient  between the free membrane potentials ,  of both neurons. In presence of a threshold mean and variance of the membrane potential determine the output firing rate  and their correlation in addition determines the output correlation , calculated by (2). B–E Direct simulation was performed using different values of common input fraction  and four fixed values of input spike synchrony  (as denoted in E). Each combination of  and  was simulated for  seconds; gray coded data points show the average over  independent realizations. Remaining parameters are given in Table 1. Solid lines in B and C are calculated as (5) and (6), respectively. In C, for convenience,  is normalized by the common input fraction , so that  in absence of synchrony (). E shows the output spike synchrony .

A pair of integrate-and-fire model neurons driven by partially shared and correlated presynaptic events. A Each of the neurons and receives input from sources, of which are excitatory and are inhibitory. Both neurons share a fraction of their excitatory and inhibitory sources, whereas the fraction is independent for each neuron. Schematically represented spike trains on the left of the diagram show the excitatory part of the input; the inhibitory input is only indicated. A single source emits spike events with a firing rate , with marginal Poisson statistics. Correlated spiking is introduced in the common excitatory sources to both neurons. This pairwise correlation is realized by means of a multiple interaction process (MIP) [39] that yields a correlation coefficient of between any pairs of sources. In absence of a threshold, the summed input drives the membrane potential to a particular working point described by its mean and standard deviation and the correlation coefficient between the free membrane potentials , of both neurons. In presence of a threshold mean and variance of the membrane potential determine the output firing rate and their correlation in addition determines the output correlation , calculated by (2). B–E Direct simulation was performed using different values of common input fraction and four fixed values of input spike synchrony (as denoted in E). Each combination of and was simulated for seconds; gray coded data points show the average over independent realizations. Remaining parameters are given in Table 1. Solid lines in B and C are calculated as (5) and (6), respectively. In C, for convenience, is normalized by the common input fraction , so that in absence of synchrony (). E shows the output spike synchrony .

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The functional significance of correlations between action potentials of neurons is still a matter of vivid debate. In particular, it is presently unclear how much synchrony is caused by afferent synchronized events and how much is intrinsic due to the connectivity structure of cortex. The available analytical approaches based on the diffusion appr...

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... [60][61][62][63]. A diverging slope of the correlation-transmission curve, shown here for binary neurons, has also been demonstrated for spiking neurons without reset [62] and for the LIF model [61,[64][65][66], suggesting that these model classes behave similarly with regard to the transition to chaos. ...
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