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Untitled - Laboratory of Neurophysics and Physiology

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internally generated propagating waves provide a specific structure for the spatiotemporal activity in<br />

visual cortex, uniquely encoding both stimulus identity <strong>and</strong> time <strong>of</strong> presentation in the amplitude <strong>and</strong><br />

phase <strong>of</strong> the population response [8]. With these results in mind, we go on to discuss the computational<br />

paradigms towards which our observations point, elucidating these with numerical models <strong>and</strong><br />

further analysis.<br />

Acknowledgements<br />

Work supported by the CNRS <strong>and</strong> the European Community (BrainScales project, FP7-269921). LM is a PhD<br />

fellow from Ècole des Neurosciences de Paris (ENP).<br />

References<br />

1. Xu W, Huang X, Takagaki K, Wu JY: Compression <strong>and</strong> reflection <strong>of</strong> visually evoked cortical waves.<br />

Neuron 2007, 55:119-129.<br />

2. Han F, Caporale N, Dan Y: Reverberation <strong>of</strong> recent visual experience in spontaneous cortical waves.<br />

Neuron 2008, 60:321-327.<br />

3. Ray S, Maunsell JH: Network rhythms influence the relationship between spike-triggered local field<br />

potential <strong>and</strong> functional connectivity. J Neurosci 2011, 31:12674-12682.<br />

4. Nauhaus I, Busse L, Ringrach DL, Car<strong>and</strong>ini M: Robustness <strong>of</strong> traveling waves in ongoing activity <strong>of</strong><br />

visual cortex. J Neurosci 2012, 32:3088-3094.<br />

5. Reynaud A, Takerkart S, Masson GS, Chavane F: Linear model decomposition for voltage-sensitive<br />

dye imaging signals: Application in awake behaving monkey. Neuroimage 2011, 54:1196-1210.<br />

6. Jancke D, Chavane F, Naaman S, Grinvald A: Imaging cortical correlates <strong>of</strong> illusion in early visual<br />

cortex. Nature 2004, 428:423-426.<br />

7. Reynaud A, Masson GS, Chavane F: Dynamics <strong>of</strong> local input normalization result from balanced<br />

short- <strong>and</strong> long-range intracortical interactions in area V1. J Neurosci 2012, 32:12558-12569.<br />

8. Ermentrout GB, Kleinfeld D: Traveling electrical waves in cortex: insights from phase dynamics <strong>and</strong><br />

speculation on a computational role. Neuron 2001, 29:33-44.<br />

O9<br />

Non-renewal spiking <strong>and</strong> neural dynamics – A simple theory <strong>of</strong> interspike interval<br />

correlations in adapting neurons<br />

Tilo Schwalger 1,2⋆ , Benjamin Lindner 1,2<br />

1 Department <strong>of</strong> Physics, Humboldt-Universität zu Berlin, Berlin, 12489, Germany<br />

2 Bernstein Center for Computational Neuroscience, Berlin, 10115, Germany<br />

There is accumulating evidence that the spiking <strong>of</strong> many neurons is not a renewal process but is<br />

characterized by correlations between interspike intervals (ISIs) [1]. These correlations are crucial for<br />

underst<strong>and</strong>ing signal processing in single neurons, however, their origin <strong>and</strong> structure is still poorly<br />

understood theoretically. Here, we present a simple theory <strong>of</strong> correlations in neural oscillators with<br />

spike-triggered adaptation currents, which are a major source <strong>of</strong> non-renewal spiking. These currents<br />

mediate spike-frequency adaptation <strong>and</strong> are commonly believed to result in negative correlations between<br />

adjacent ISIs. For such adapting neurons, we show that the serial correlation coefficient (SCC)<br />

is fundamentally related to the neuron’s phase response curve (PRC). The relation predicts possible<br />

correlation patterns that characterize how correlations depend on the lag between ISIs. Different patterns<br />

arise from the specific interplay between nonlinear neural dynamics <strong>and</strong> adaptation dynamics. In<br />

particular, the correlation structure can be determined by a single parameter that includes the shape<br />

<strong>of</strong> the PRC as well as the strength <strong>and</strong> time scale <strong>of</strong> the adaptation current (Fig. 1).<br />

For a positive PRC (type I), the SCC is always negative at lag 1. At higher lags, we find either a<br />

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