2011
DOI: 10.1103/physreve.83.061916
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Optimal design of minimum-power stimuli for phase models of neuron oscillators

Abstract: In this paper, we study optimal control problems of spiking neurons whose dynamics are described by a phase model. We design minimum-power current stimuli (controls) that lead to targeted spiking times. In particular, we consider bounded control amplitude and characterize the range of possible spiking times determined by the bound, which can be chosen sufficiently small within the range where the phase model is valid. We show that for a given bound the corresponding feasible spiking times are optimally achieve… Show more

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Cited by 65 publications
(67 citation statements)
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“…where α is a constant defined in (12). Since the minimum-time control takes the bangbang form as shown in Section 2.1.1, it requires to calculate the switching points and determine the type of the switching at these points for the optimal control synthesis.…”
Section: Discussionmentioning
confidence: 99%
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“…where α is a constant defined in (12). Since the minimum-time control takes the bangbang form as shown in Section 2.1.1, it requires to calculate the switching points and determine the type of the switching at these points for the optimal control synthesis.…”
Section: Discussionmentioning
confidence: 99%
“…It has been observed through experiments that the PRC for an Aplysia motoneuron is extremely similar to that of a Morris-Lecar PRC [29]. We consider a Morris-Lecar system with parameter values given in [12], which has a natural frequency ω = 0.283 rad/ms. The PRC is approximated by (26) with the coefficients shown in Table 2 and is illustrated, with its derivatives, in Figure 5 Table 2.…”
Section: Morris-lecar Phase Modelmentioning
confidence: 99%
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“…[8,9,17,25], optimal forcings have been designed for various purposes and constraints. Their arguments are all based on variational calculus, such as the Euler-Lagrange equation [26] or Pontryagin's minimum principle [27].…”
Section: Resultsmentioning
confidence: 99%
“…The constraints in Eq. (9) imply that there exists an upper bound of J[f ], i.e., the ideal locking range R[f ] under the constraints of (4) and (5). In addition, for the case of 1 < p < ∞ mentioned above, the equality condition has to be satisfied for this ideal locking range to be realized.…”
Section: Some Properties Derived From Hölder's Inequality In Preparatmentioning
confidence: 97%