2020
DOI: 10.48550/arxiv.2007.15174
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Learning interaction kernels in stochastic systems of interacting particles from multiple trajectories

Abstract: We consider stochastic systems of interacting particles or agents, with dynamics determined by an interaction kernel which only depends on pairwise distances. We study the problem of inferring this interaction kernel from observations of the positions of the particles, in either continuous or discrete time, along multiple independent trajectories. We introduce a nonparametric inference approach to this inverse problem, based on a regularized maximum likelihood estimator constrained to suitable hypothesis space… Show more

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Cited by 2 publications
(5 citation statements)
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“…The positivity of c H K is related to the positivity of relevant integral operators. Leveraging the recent advancement in [31,32], our ongoing work shows that, in the case of L = 1, the coercivity constant c H K ≥ N −1 N 2 for general systems and H K . Furthermore, it can be a positive constant independent of N if µ 0 is exchangeable Gaussian.…”
Section: J ρLmentioning
confidence: 89%
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“…The positivity of c H K is related to the positivity of relevant integral operators. Leveraging the recent advancement in [31,32], our ongoing work shows that, in the case of L = 1, the coercivity constant c H K ≥ N −1 N 2 for general systems and H K . Furthermore, it can be a positive constant independent of N if µ 0 is exchangeable Gaussian.…”
Section: J ρLmentioning
confidence: 89%
“…The learning theory developed in this paper is related to but significantly departs from the ones for the previous approach [29,[31][32][33]. All of these works investigate the performance of estimators as M → ∞.…”
Section: Comparison With Previous Workmentioning
confidence: 99%
“…Note that s ρ T depends on the initial distribution up¨, 0q and the true interaction kernel φ. We point out that the measure s ρ T is different from the empirical measure of pairwise distances in particle systems [22,21,19], because s X t and s X 1 t are independent copies and are no longer interacting particles. However, in view of inference, the high probability region of s ρ T is where ˇˇs X t ´s X 1 t ˇˇexplores the interaction kernel the most, as such, the natural function space of inference is L 2 ps ρ T q.…”
Section: The Error Functional and Estimatormentioning
confidence: 88%
“…When these basis functions are orthonormal in L 2 ps ρ T q, we need the following coercivity condition. It extends of the coercivity condition for Nparticle systems defined in [19,21,22]. Definition 3.3 (Coercivity condition).…”
Section: Convergence Of the Estimator In Mesh Sizementioning
confidence: 99%
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