Antithetic multilevel particle system sampling method for McKean-Vlasov SDEs

Let \(\mu\in \mathcal{P}_2(\mathbb R^d)\), where \(\mathcal{P}_2(\mathbb R^d)\) denotes the space of square integrable probability measures, and consider a Borel-measurable function \(\Phi:\mathcal P_2(\mathbb R^d)\rightarrow \mathbb R \). IIn this paper we develop Antithetic Monte Carlo estimator (...

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Veröffentlicht in:arXiv.org 2021-04
Hauptverfasser: Szpruch, Łukasz, Tse, Alvin
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Sprache:eng
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Zusammenfassung:Let \(\mu\in \mathcal{P}_2(\mathbb R^d)\), where \(\mathcal{P}_2(\mathbb R^d)\) denotes the space of square integrable probability measures, and consider a Borel-measurable function \(\Phi:\mathcal P_2(\mathbb R^d)\rightarrow \mathbb R \). IIn this paper we develop Antithetic Monte Carlo estimator (A-MLMC) for \(\Phi(\mu)\), which achieves sharp error bound under mild regularity assumptions. The estimator takes as input the empirical laws \(\mu^N = \frac1N \sum_{i=1}^{N}\delta_{X_i}\), where a) \((X_i)_{i=1}^N\) is a sequence of i.i.d samples from \(\mu\) or b) \((X_i)_{i=1}^N\) is a system of interacting particles (diffusions) corresponding to a McKean-Vlasov stochastic differential equation (McKV-SDE). Each case requires a separate analysis. For a mean-field particle system, we also consider the empirical law induced by its Euler discretisation which gives a fully implementable algorithm. As by-products of our analysis, we establish a dimension-independent rate of uniform \textit{strong propagation of chaos}, as well as an \(L^2\) estimate of the antithetic difference for i.i.d. random variables corresponding to general functionals defined on the space of probability measures.
ISSN:2331-8422
DOI:10.48550/arxiv.1903.07063