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Abstracts of Posters 8-th European Conference on Mathematical ...

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<str<strong>on</strong>g>European</str<strong>on</strong>g> <str<strong>on</strong>g>C<strong>on</strong>ference</str<strong>on</strong>g> <strong>on</strong> Ma<str<strong>on</strong>g>th</str<strong>on</strong>g>ematical and Theoretical Biology 2011<br />

Poster Sessi<strong>on</strong>; Friday, July 1, 20:00<br />

Peter Rowat<br />

Institute for Neural Computati<strong>on</strong>, University <str<strong>on</strong>g>of</str<strong>on</strong>g> California San Diego,<br />

USA<br />

e-mail: prowat@ucsd.edu<br />

Priscilla Greenwood<br />

Department <str<strong>on</strong>g>of</str<strong>on</strong>g> Ma<str<strong>on</strong>g>th</str<strong>on</strong>g>ematics, University <str<strong>on</strong>g>of</str<strong>on</strong>g> British Columbia, Vancouver,<br />

BC, Canada<br />

Identificati<strong>on</strong> and c<strong>on</strong>tinuity <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>e distributi<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

burst-leng<str<strong>on</strong>g>th</str<strong>on</strong>g> and inter-spike-intervals in <str<strong>on</strong>g>th</str<strong>on</strong>g>e stochastic<br />

Morris-Lecar neur<strong>on</strong><br />

Using <str<strong>on</strong>g>th</str<strong>on</strong>g>e Morris-Lecar model neur<strong>on</strong> wi<str<strong>on</strong>g>th</str<strong>on</strong>g> a type II parameter set and K+ channel<br />

noise, we investigate <str<strong>on</strong>g>th</str<strong>on</strong>g>e inter-spike interval distributi<strong>on</strong> as increasing levels <str<strong>on</strong>g>of</str<strong>on</strong>g> applied<br />

current drive <str<strong>on</strong>g>th</str<strong>on</strong>g>e model <str<strong>on</strong>g>th</str<strong>on</strong>g>rough a sub-critical Hopf bifurcati<strong>on</strong>. Our goal was<br />

to provide a quantitative descripti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>e distributi<strong>on</strong>s associated wi<str<strong>on</strong>g>th</str<strong>on</strong>g> spiking as<br />

a functi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> applied current. The model generates bursty spiking behavior wi<str<strong>on</strong>g>th</str<strong>on</strong>g><br />

sequences <str<strong>on</strong>g>of</str<strong>on</strong>g> random numbers <str<strong>on</strong>g>of</str<strong>on</strong>g> spikes (bursts) separated by inter-burst intervals<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> random leng<str<strong>on</strong>g>th</str<strong>on</strong>g>. This kind <str<strong>on</strong>g>of</str<strong>on</strong>g> spiking behavior is found in many places in <str<strong>on</strong>g>th</str<strong>on</strong>g>e nervous<br />

system, most notably, perhaps, in stuttering inhibitory interneur<strong>on</strong>s in cortex.<br />

Here we show several practical and inviting aspects <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>is model, combining analysis<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>e stochastic dynamics <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>e model wi<str<strong>on</strong>g>th</str<strong>on</strong>g> estimati<strong>on</strong> based <strong>on</strong> simulati<strong>on</strong>s.<br />

We show <str<strong>on</strong>g>th</str<strong>on</strong>g>at <str<strong>on</strong>g>th</str<strong>on</strong>g>e parameter <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>e exp<strong>on</strong>ential tail <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>e ISI distributi<strong>on</strong> is in<br />

fact c<strong>on</strong>tinuous over <str<strong>on</strong>g>th</str<strong>on</strong>g>e entire range <str<strong>on</strong>g>of</str<strong>on</strong>g> plausible applied current, regardless <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>e<br />

bifurcati<strong>on</strong>s in <str<strong>on</strong>g>th</str<strong>on</strong>g>e phase-portrait <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>th</str<strong>on</strong>g>e model. Fur<str<strong>on</strong>g>th</str<strong>on</strong>g>er, we show <str<strong>on</strong>g>th</str<strong>on</strong>g>at <str<strong>on</strong>g>th</str<strong>on</strong>g>e spike<br />

sequence leng<str<strong>on</strong>g>th</str<strong>on</strong>g>, apparently studied for <str<strong>on</strong>g>th</str<strong>on</strong>g>e first time here, has a geometric distributi<strong>on</strong><br />

whose associated parameter is c<strong>on</strong>tinuous as a functi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> applied current<br />

over <str<strong>on</strong>g>th</str<strong>on</strong>g>e entire input range. Hence <str<strong>on</strong>g>th</str<strong>on</strong>g>is model is applicable over a much wider range<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> applied current <str<strong>on</strong>g>th</str<strong>on</strong>g>an has been <str<strong>on</strong>g>th</str<strong>on</strong>g>ought.<br />

842

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