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Yamada, W.M.1
Koch, C.2
Adams, P.R.3
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2
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0002331710
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edited by D. Touretzky (Morgan Kaufmann, San Mateo, CA)
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M.A. Wilson, U.S. Bhalla, J.D. Uhley, and J.M. Brower, in Advances in Neuronal Information Processing Systems, edited by D. Touretzky (Morgan Kaufmann, San Mateo, CA, 1989), pp. 485-492.
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Wilson, M.A.1
Bhalla, U.S.2
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12
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0002453062
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edited by C. Koch and I. Segev (MIT Press, Cambridge, MA)
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J. Rinzel and G.B. Ermentrout, in Methods in Neuronal Modeling: From Ions to Networks, 2nd ed., edited by C. Koch and I. Segev (MIT Press, Cambridge, MA, 1998), pp. 251-291.
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Rinzel, J.1
Ermentrout, G.B.2
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17
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77956761866
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edited by F. Moss and S. Gielen (Elsevier Science, Amsterdam)
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W. Gerstner, in The Handbook of Biological Physics, edited by F. Moss and S. Gielen (Elsevier Science, Amsterdam, 2001), Vol 4, pp. 469-516.
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Gerstner, W.1
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27
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33645077580
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note
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One can easily generalize the definitions of the two sets for noncontinuous dynamics of the membrane potential.
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28
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33645077844
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note
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Note that the leaky integrator neuron presents a resonant behavior when b>0.
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29
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33645059141
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note
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The case γ=0 is not interesting since a rescaling of w allows to set I = 0.
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30
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33645076755
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note
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An additional bifurcation occurs for a particular range of γ values (not shown in Fig. 7). This bifurcation is a double homoclinic bifurcation which appears when the two unstable periodic solutions with sliding motion bifurcates from an unstable periodic solution. These two unstable limit cycles surround the two fixed points, respectively, and become simultaneously homoclinic to a degenerate saddle point along the line of discontinuity (as the bifurcation point is reached). We do not analyze this situation since unstable cycles are not directly observable.
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33
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0003490410
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Addison-Wesley, Reading, MA
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S.H. Strogatz, Nonlinear Dynamics and Chaos. With Application to Physics, Biology, Chemistry and Engineering (Addison-Wesley, Reading, MA, 1994).
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(1994)
Nonlinear Dynamics and Chaos. With Application to Physics, Biology, Chemistry and Engineering
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Strogatz, S.H.1
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