Second order interlaced polynomial lattice rules for integration over $\mathbb{R}^s$

We study numerical integration of functions $f: \mathbb{R}^{s} \to \mathbb{R}$ with respect to a probability measure. By applying the corresponding inverse cumulative distribution function, the problem is transformed into integrating an induced function over the unit cube $(0,1)^{s}$. We introduce a new orthonormal system: \emph{order~2 localized Walsh functions}. These basis functions retain the approximation power of classical Walsh functions for twice-differentiable integrands while inheriting the spatial localization of Haar wavelets. Localization is crucial because the transformed integrand is typically unbounded at the boundary. We show that the worst-case quasi-Monte Carlo integration error decays like $\mathcal{O}(N^{-1/λ})$ for every $λ\in (1/2,1]$. As an application, we consider elliptic partial differential equations with a finite number of log-normal random coefficients and show that our error estimates remain valid for their stochastic Galerkin discretizations by applying a suitable importance sampling density.

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Journal
ArXiv.org
Published
2025-09-30
Primary Topic
Mathematical Approximation and Integration
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article
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article

Second order interlaced polynomial lattice rules for integration over $\mathbb{R}^s$

ArXiv.org
Mathematical Approximation and Integration
article

Second order interlaced polynomial lattice rules for integration over $\mathbb{R}^s$

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Abstract

We study numerical integration of functions $f: \mathbb{R}^{s} \to \mathbb{R}$ with respect to a probability measure. By applying the corresponding inverse cumulative distribution function, the problem is transformed into integrating an induced function over the unit cube $(0,1)^{s}$. We introduce a new orthonormal system: \emph{order~2 localized Walsh functions}. These basis functions retain the approximation power of classical Walsh functions for twice-differentiable integrands while inheriting the spatial localization of Haar wavelets. Localization is crucial because the transformed integrand is typically unbounded at the boundary. We show that the worst-case quasi-Monte Carlo integration error decays like $\mathcal{O}(N^{-1/λ})$ for every $λ\in (1/2,1]$. As an application, we consider elliptic partial differential equations with a finite number of log-normal random coefficients and show that our error estimates remain valid for their stochastic Galerkin discretizations by applying a suitable importance sampling density.

ArXiv.org
Openalex Percentile: Top 35%
Mathematical Approximation and Integration
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Second order interlaced polynomial lattice rules for integration over $\mathbb{R}^s$ · ArXiv.org (2025) | TGRS Research Map | TGRS