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The result of simulations of the first-passage time distribution for a discretized equation x ͑ t + 1 ͒ = x ͑ t ͒ + dt ͑ ␮ x ͑ t − ␶ ͒ + ␰ ͒ where ␰ is a Gaussian white noise with variance ␴ 2 . We have set the threshold at X = 5.0. The 

The result of simulations of the first-passage time distribution for a discretized equation x ͑ t + 1 ͒ = x ͑ t ͒ + dt ͑ ␮ x ͑ t − ␶ ͒ + ␰ ͒ where ␰ is a Gaussian white noise with variance ␴ 2 . We have set the threshold at X = 5.0. The 

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The inverted pendulum is frequently used as a starting point for discussions of how human balance is maintained during standing and locomotion. Here we examine three experimental paradigms of time-delayed balance control: (1) mechanical inverted time-delayed pendulum, (2) stick balancing at the fingertip, and (3) human postural sway during quiet st...

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... of a first-passage time problem for an unstable fixed point left- hand side of Eq. 15 with reinjection into the interval − − wherever the threshold is crossed. Current interest has focused on the possibility that the left-hand side of Eq. 15 also contains a time delay. This gives rise to a unstable delayed random walk. 32,35,38 As is shown in Fig. 3, the interplay between noise and delay can transiently stabilize the unstable fixed point, i.e., prolong the first-passage time. These effects are interesting in light of measurements of the reaction time and response time when posture is perturbed. 46 In this study it was observed that the neural time delay, i.e., the time interval ...

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