{"title":"A degenerate version of Brion's formula","authors":"Carsten Peterson","doi":"arxiv-2409.09544","DOIUrl":null,"url":null,"abstract":"Let $\\mathfrak{p} \\subset V$ be a polytope and $\\xi \\in V_{\\mathbb{C}}^*$. We\nobtain an expression for $I(\\mathfrak{p}; \\alpha) := \\int_{\\mathfrak{p}}\ne^{\\langle \\alpha, x \\rangle} dx$ as a sum of meromorphic functions in $\\alpha\n\\in V^*_{\\mathbb{C}}$ parametrized by the faces $\\mathfrak{f}$ of\n$\\mathfrak{p}$ on which $\\langle \\xi, x \\rangle$ is constant. Each term only\ndepends on the local geometry of $\\mathfrak{p}$ near $\\mathfrak{f}$ (and on\n$\\xi$) and is holomorphic at $\\alpha = \\xi$. When $\\langle \\xi, \\cdot \\rangle$\nis only constant on the vertices of $\\mathfrak{p}$ our formula reduces to\nBrion's formula. Suppose $\\mathfrak{p}$ is a rational polytope with respect to a lattice\n$\\Lambda$. We obtain an expression for $S(\\mathfrak{p}; \\alpha) :=\n\\sum_{\\lambda \\in \\mathfrak{p} \\cap \\Lambda} e^{\\langle \\alpha, \\lambda\n\\rangle}$ as a sum of meromorphic functions parametrized by the faces\n$\\mathfrak{f}$ on which $e^{\\langle \\xi, x \\rangle} = 1$ on a finite index\nsublattice of $\\text{lin}(\\mathfrak{f}) \\cap \\Lambda$. Each term only depends\non the local geometry of $\\mathfrak{p}$ near $\\mathfrak{f}$ (and on $\\xi$ and\n$\\Lambda$) and is holomorphic at $\\alpha = \\xi$. When $e^{\\langle \\xi, \\cdot\n\\rangle} \\neq 1$ at any non-zero lattice point on a line through the origin\nparallel to an edge of $\\mathfrak{p}$, our formula reduces to Brion's formula,\nand when $\\xi = 0$, it reduces to the Ehrhart quasi-polynomial. Our formulas are particularly useful for understanding how\n$I(\\mathfrak{p}(h); \\xi)$ and $S(\\mathfrak{p}(h); \\xi)$ vary in a family of\npolytopes $\\mathfrak{p}(h)$ with the same normal fan. When considering dilates\nof a fixed polytope, our formulas may be viewed as polytopal analogues of\nLaplace's method and the method of stationary phase. Such expressions naturally\nshow up in analysis on symmetric spaces and affine buildings.","PeriodicalId":501407,"journal":{"name":"arXiv - MATH - Combinatorics","volume":"70 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - MATH - Combinatorics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.09544","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Let $\mathfrak{p} \subset V$ be a polytope and $\xi \in V_{\mathbb{C}}^*$. We
obtain an expression for $I(\mathfrak{p}; \alpha) := \int_{\mathfrak{p}}
e^{\langle \alpha, x \rangle} dx$ as a sum of meromorphic functions in $\alpha
\in V^*_{\mathbb{C}}$ parametrized by the faces $\mathfrak{f}$ of
$\mathfrak{p}$ on which $\langle \xi, x \rangle$ is constant. Each term only
depends on the local geometry of $\mathfrak{p}$ near $\mathfrak{f}$ (and on
$\xi$) and is holomorphic at $\alpha = \xi$. When $\langle \xi, \cdot \rangle$
is only constant on the vertices of $\mathfrak{p}$ our formula reduces to
Brion's formula. Suppose $\mathfrak{p}$ is a rational polytope with respect to a lattice
$\Lambda$. We obtain an expression for $S(\mathfrak{p}; \alpha) :=
\sum_{\lambda \in \mathfrak{p} \cap \Lambda} e^{\langle \alpha, \lambda
\rangle}$ as a sum of meromorphic functions parametrized by the faces
$\mathfrak{f}$ on which $e^{\langle \xi, x \rangle} = 1$ on a finite index
sublattice of $\text{lin}(\mathfrak{f}) \cap \Lambda$. Each term only depends
on the local geometry of $\mathfrak{p}$ near $\mathfrak{f}$ (and on $\xi$ and
$\Lambda$) and is holomorphic at $\alpha = \xi$. When $e^{\langle \xi, \cdot
\rangle} \neq 1$ at any non-zero lattice point on a line through the origin
parallel to an edge of $\mathfrak{p}$, our formula reduces to Brion's formula,
and when $\xi = 0$, it reduces to the Ehrhart quasi-polynomial. Our formulas are particularly useful for understanding how
$I(\mathfrak{p}(h); \xi)$ and $S(\mathfrak{p}(h); \xi)$ vary in a family of
polytopes $\mathfrak{p}(h)$ with the same normal fan. When considering dilates
of a fixed polytope, our formulas may be viewed as polytopal analogues of
Laplace's method and the method of stationary phase. Such expressions naturally
show up in analysis on symmetric spaces and affine buildings.