<p>(A) The depression <i>μ</i> is plotted on the <i>x</i>-axis, while the variable <i>V</i> is on the <i>y</i>-axis (for the schematic representation, no scale is given). The recurrent sets are the attractor points <i>P</i><sub>1</sub> (the Down state), the saddle point <i>P</i><sub>3</sub><b>,</b> and the attractor <i>P</i><sub>2</sub> (the Up state), separated by an unstable limit cycle C (dashed line). The region inside the unstable limit cycle is the basin of attraction of <i>P</i><sub>2</sub>. By definition, it is the Up state. For a specific value of the parameter, an homoclinic curve can appear. The unstable branch of the separatrix starting from <i>P</i><sub>3</sub> terminates inside the basin of attraction of the Down state. The no...
<p>Upper left: Single neuron (<i>α</i> = 0.7, <i>V</i><sub>0</sub> = 6.2mV) firing once after stimul...
A) Poincaré maps illustrate that the cycles of Fig 2 correspond to attractive limit cycles. Sixteen ...
<p>This figure shows the probabilities of each basin of attraction in the phase space (vertical axis...
<p><b>A</b>) A schematic showing the mood change as a function of the state variable <i>M</i> withou...
<p>(a) and (b) represent critical transitions without and with noise in the attractor dynamics, resp...
<p>(A–C) Schematic drawings of a limit cycle attractor and a perturbation delivered to the system ar...
<p>(a) for <i>ϵ</i> < 1/4 and (b) for <i>ϵ</i> > 1/4. Stable equilibria are marked by a red circle, ...
<p>(A) A typical realization of Up–Down transition dynamics in the stochastic model with <i>w<sub>T<...
<p>(a) Time evolution of <i>v</i>(<i>t</i>). (b) Its trajectory in the (<i>v</i>, <i>u</i>) phase pl...
<p><i>A</i> = 3, <i>β</i> = 0.375, <i>α</i> = 0.5, <i>μ</i><sub>0</sub> = 0.5, <i>μ</i><sub>1</sub> ...
<p><i>I</i> = 90.7 μA/cm<sup>2</sup> and <i>V</i><sub><i>K</i></sub> = -84 mV. (a) The stable focus ...
<p>A-D: P(C) for trials when the sure target was (not) shown are represented with filled (open) circ...
<p>(A) Schematic representation of how the signal modifies the trajectories of G1-phase progression...
<p>a) Three equilibriums may occur at intersection points where the rate of generation of new pulses...
<div><p>The <i>x</i> nullcline, the <i>u</i> nullcline, and the forbidden line (<i>Jux</i> = 1) are ...
<p>Upper left: Single neuron (<i>α</i> = 0.7, <i>V</i><sub>0</sub> = 6.2mV) firing once after stimul...
A) Poincaré maps illustrate that the cycles of Fig 2 correspond to attractive limit cycles. Sixteen ...
<p>This figure shows the probabilities of each basin of attraction in the phase space (vertical axis...
<p><b>A</b>) A schematic showing the mood change as a function of the state variable <i>M</i> withou...
<p>(a) and (b) represent critical transitions without and with noise in the attractor dynamics, resp...
<p>(A–C) Schematic drawings of a limit cycle attractor and a perturbation delivered to the system ar...
<p>(a) for <i>ϵ</i> < 1/4 and (b) for <i>ϵ</i> > 1/4. Stable equilibria are marked by a red circle, ...
<p>(A) A typical realization of Up–Down transition dynamics in the stochastic model with <i>w<sub>T<...
<p>(a) Time evolution of <i>v</i>(<i>t</i>). (b) Its trajectory in the (<i>v</i>, <i>u</i>) phase pl...
<p><i>A</i> = 3, <i>β</i> = 0.375, <i>α</i> = 0.5, <i>μ</i><sub>0</sub> = 0.5, <i>μ</i><sub>1</sub> ...
<p><i>I</i> = 90.7 μA/cm<sup>2</sup> and <i>V</i><sub><i>K</i></sub> = -84 mV. (a) The stable focus ...
<p>A-D: P(C) for trials when the sure target was (not) shown are represented with filled (open) circ...
<p>(A) Schematic representation of how the signal modifies the trajectories of G1-phase progression...
<p>a) Three equilibriums may occur at intersection points where the rate of generation of new pulses...
<div><p>The <i>x</i> nullcline, the <i>u</i> nullcline, and the forbidden line (<i>Jux</i> = 1) are ...
<p>Upper left: Single neuron (<i>α</i> = 0.7, <i>V</i><sub>0</sub> = 6.2mV) firing once after stimul...
A) Poincaré maps illustrate that the cycles of Fig 2 correspond to attractive limit cycles. Sixteen ...
<p>This figure shows the probabilities of each basin of attraction in the phase space (vertical axis...