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Gibbs flow for approximate transport with applications to Bayesian computation

29 September 2015
J. Heng
Arnaud Doucet
Y. Pokern
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Abstract

Let π0\pi_{0}π0​ and π1\pi_{1}π1​ be two distributions on the Borel space (Rd,B(Rd))(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d}))(Rd,B(Rd)). Any measurable function T:Rd→RdT:\mathbb{R}^{d}\rightarrow\mathbb{R}^{d}T:Rd→Rd such that Y=T(X)∼π1Y=T(X)\sim\pi_{1}Y=T(X)∼π1​ if X∼π0X\sim\pi_{0}X∼π0​ is called a transport map from π0\pi_{0}π0​ to π1\pi_{1}π1​. For any π0\pi_{0}π0​ and π1\pi_{1}π1​, if one could obtain an analytical expression for a transport map from π0\pi_{0}π0​ to π1\pi_{1}π1​, then this could be straightforwardly applied to sample from any distribution. One would map draws from an easy-to-sample distribution π0\pi_{0}π0​ to the target distribution π1\pi_{1}π1​ using this transport map. Although it is usually impossible to obtain an explicit transport map for complex target distributions, we show here how to build a tractable approximation of a novel transport map. This is achieved by moving samples from π0\pi_{0}π0​ using an ordinary differential equation with a velocity field that depends on the full conditional distributions of the target. Even when this ordinary differential equation is time-discretized and the full conditional distributions are numerically approximated, the resulting distribution of mapped samples can be efficiently evaluated and used as a proposal within sequential Monte Carlo samplers. We demonstrate significant gains over state-of-the-art sequential Monte Carlo samplers at a fixed computational complexity on a variety of applications.

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