Abstract:We present an approximate analytical expression for escape rates of time-dependent driven stochastic processes with an absorbing boundary such as the driven leaky integrate-and-fire model for neural spiking. The novel approximation is based on a discrete state Markovian modeling of the full long-time dynamics with time-dependent rates. It is valid in a wide parameter regime beyond the restraining limits of weak driving (linear response) and/or weak noise. The scheme is carefully tested and yields excellent agr… Show more
“…For example, fluctuations around the MFPT, quantified by the second moment, provide a measure of the number of detections needed to collect a reliable statistics for the FPT analysis. The FPT pdf also determines the so-termed residence time and interspike pdfs, which generally are more readily available in experiments, e.g., in the context of stochastic resonance phenomena [39], and involve suitable averages over the FPT pdf [6,21,37,38]. The residence time pdf is explicitly evaluated in Sec.…”
Quantum resonant activation is investigated for the archetype setup of an externally driven two-state (spinboson) system subjected to strong dissipation by means of both analytical and extensive numerical calculations. The phenomenon of resonant activation emerges in the presence of either randomly fluctuating or deterministic periodically varying driving fields. Addressing the incoherent regime, a characteristic minimum emerges in the mean first passage time to reach an absorbing neighboring state whenever the intrinsic time scale of the modulation matches the characteristic time scale of the system dynamics. For the case of deterministic periodic driving, the first passage time probability density function (pdf) displays a complex, multipeaked behavior, which depends crucially on the details of initial phase, frequency, and strength of the driving. As an interesting feature we find that the mean first passage time enters the resonant activation regime at a critical frequency ν * which depends very weakly on the strength of the driving. Moreover, we provide the relation between the first passage time pdf and the statistics of residence times.
“…For example, fluctuations around the MFPT, quantified by the second moment, provide a measure of the number of detections needed to collect a reliable statistics for the FPT analysis. The FPT pdf also determines the so-termed residence time and interspike pdfs, which generally are more readily available in experiments, e.g., in the context of stochastic resonance phenomena [39], and involve suitable averages over the FPT pdf [6,21,37,38]. The residence time pdf is explicitly evaluated in Sec.…”
Quantum resonant activation is investigated for the archetype setup of an externally driven two-state (spinboson) system subjected to strong dissipation by means of both analytical and extensive numerical calculations. The phenomenon of resonant activation emerges in the presence of either randomly fluctuating or deterministic periodically varying driving fields. Addressing the incoherent regime, a characteristic minimum emerges in the mean first passage time to reach an absorbing neighboring state whenever the intrinsic time scale of the modulation matches the characteristic time scale of the system dynamics. For the case of deterministic periodic driving, the first passage time probability density function (pdf) displays a complex, multipeaked behavior, which depends crucially on the details of initial phase, frequency, and strength of the driving. As an interesting feature we find that the mean first passage time enters the resonant activation regime at a critical frequency ν * which depends very weakly on the strength of the driving. Moreover, we provide the relation between the first passage time pdf and the statistics of residence times.
“…Either numerical methods have to be used or in specific cases, tailored approximations may be applied in order to analyze relevant aspects of the dynamical behavior of the model [7][8][9]4]. The numerical methods either deal with the stochastic differential equations [10,11] or the equivalent Fokker-Planck equation [11][12][13]. For time dependent Ornstein-Uhlenbeck processes the first passage time density can also be obtained from an integral equation [14], which provides a convenient starting point for numerical investigations [15,13].…”
Section: Introductionmentioning
confidence: 99%
“…The numerical methods either deal with the stochastic differential equations [10,11] or the equivalent Fokker-Planck equation [11][12][13]. For time dependent Ornstein-Uhlenbeck processes the first passage time density can also be obtained from an integral equation [14], which provides a convenient starting point for numerical investigations [15,13].…”
Section: Introductionmentioning
confidence: 99%
“…For the slow subthreshold driving considered here we may follow the line of reasoning that was applied to the linear leaky integrate-and-fire model [12,13] and outlined in Ref. [18] in more detail.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, the primary task is to find the firing rate. For weak noise and slow driving frequencies the time dependent rates are given by the values of the rates at the instantaneous driving strength [18,12,13,19].…”
Statistical properties of neuron firing are studied in the framework of a nonlinear leaky integrate-and-fire model that is driven by a slow periodic subthreshold signal. The firing events are characterized by first passage time densities. The experimentally better accessible interspike interval density generally depends on the sojourn times in a refractory state of the neuron. This aspect is not part of the integrate-and-fire model and must be modelled additionally. For a large class of refractory dynamics, a general expression for the interspike interval density is given and further evaluated for the two cases with an instantaneous resetting (i.e. no refractory state) and a refractory state possessing a deterministic lifetime. First passage time densities and interspike interval densities following from the proposed theory compare favorably with precise numerical simulations.
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