2014
DOI: 10.1016/j.physd.2013.12.007
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A Kushner–Stratonovich Monte Carlo filter applied to nonlinear dynamical system identification

Abstract: A Monte Carlo filter, based on the idea of averaging over characteristics and fashioned after a particle-based time-discretized approximation to the Kushner-Stratonovich (KS) nonlinear filtering equation, is proposed. A key aspect of the new filter is the gain-like additive update, designed to approximate the innovation integral in the KS equation and implemented through an annealing-type iterative procedure, which is aimed at rendering the innovation (observation-prediction mismatch) for a given time-step to … Show more

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Cited by 15 publications
(13 citation statements)
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“…However an exact solution of the KS equation is available only under the restriction of a linear measurement operator and the assumption that the noises involved are Gaussian. An attempt has been made to solve a discretized version of the KS equation in a Monte Carlo setting [26] that provides an additive correction to each predicted realization of the parameter process. The additive gain-like term is arrived at using tools from stochastic calculus and the detailed derivation of the same is provided in [22].…”
Section: Evolutionary Stochastic Reconstruction Methodsmentioning
confidence: 99%
“…However an exact solution of the KS equation is available only under the restriction of a linear measurement operator and the assumption that the noises involved are Gaussian. An attempt has been made to solve a discretized version of the KS equation in a Monte Carlo setting [26] that provides an additive correction to each predicted realization of the parameter process. The additive gain-like term is arrived at using tools from stochastic calculus and the detailed derivation of the same is provided in [22].…”
Section: Evolutionary Stochastic Reconstruction Methodsmentioning
confidence: 99%
“…Even with scrambling and blending, a search scheme that always chooses to update the particles would The dimensionality curse, which besets many stochastic search schemes including most stochastic filters with the necessity of an exponentially exploding ensemble size, comes in the way of solving inverse problems with a large number of unknowns. To a large extent, the particle degeneracy problems encountered by weight-based schemes are circumvented in the additive-update strategies that attempt at 'healing' the bad particles instead of eliminating them altogether [7]. However, even with such an approach, the quality of solutions is highly dependent on the ensemble size, e n , as has been proved in [24].…”
Section: Relaxation and Selectionmentioning
confidence: 99%
“…Neglecting contributions from tr ∇uR T ∇uR T and tr(RR) T , the discrete Hamiltonian finally takes the following form. The governing dynamics for the system and bath variables, described through Hamilton's equations in terms of the displacement DOFs and the momenta, are given by the equation pairs (11,12) and (13,14) …”
Section: Formulation Of Discrete Hamiltonianmentioning
confidence: 99%
“…In Fig.2, we also see that simulation using the standard GLE fails to produce the steady-state fluctuations. The proposed GLE is further tested in the context of an inverse problem, wherein using it as a process model, a stochastic projection on the experimental MSD data through a nonlinear filter [13] leads to an estimate quite close to the measurement (Fig.3). However, the same exercise with the standard GLE as process model (for the same Monte Carlo sample size) produces a completely different response estimate.…”
mentioning
confidence: 99%