齐次流形上构造不变偏微分方程的一般方法

D. Alekseevsky, J. Gutt, G. Manno, G. Moreno
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引用次数: 2

摘要

设$M = G/H$为$(n+1)$维齐次流形,$J^k(n,M)=:J^k$为$M$的超曲面的$k$ -射流流形。李群$G$自然作用于每个$J^k$。对于$M$的超曲面(即具有$n$自变量和$1$依赖变量),其阶为$k$的$G$不变PDE被定义为$G$不变超曲面$\mathcal{E} \subset J^k$。我们描述了一种构造$k\geq 2$不变偏微分方程的一般方法。该问题归结为在一定向量空间中对$G$的$(k-1)$ -延长作用的稳定性子群$H^{(k-1)}$的线性作用不变的超曲面的描述。我们将此方法应用于描述欧氏空间$\mathbb{E}^{n+1 }$和保形空间$\mathbb{S}^{n+1}$中超曲面的不变偏微分方程。我们的方法是在对$G$的作用的一些温和假设下工作的,即:A1)基团$G$必须在$J^{k-1}$中有一个开轨道,A2)纤维的稳定剂$H^{(k-1)}\subset G$$J^k\to J^{k-1}$必须通过纤维本身的平移组来分解。
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A general method to construct invariant PDEs on homogeneous manifolds
Let $M = G/H$ be an $(n+1)$-dimensional homogeneous manifold and $J^k(n,M)=:J^k$ be the manifold of $k$-jets of hypersurfaces of $M$. The Lie group $G$ acts naturally on each $J^k$. A $G$-invariant PDE of order $k$ for hypersurfaces of $M$ (i.e., with $n$ independent variables and $1$ dependent one) is defined as a $G$-invariant hypersurface $\mathcal{E} \subset J^k$. We describe a general method for constructing such invariant PDEs for $k\geq 2$. The problem reduces to the description of hypersurfaces, in a certain vector space, which are invariant with respect to the linear action of the stability subgroup $H^{(k-1)}$ of the $(k-1)$-prolonged action of $G$. We apply this approach to describe invariant PDEs for hypersurfaces in the Euclidean space $\mathbb{E}^{n+1 }$ and in the conformal space $\mathbb{S}^{n+1}$. Our method works under some mild assumptions on the action of $G$, namely: A1) the group $G$ must have an open orbit in $J^{k-1}$, and A2) the stabilizer $H^{(k-1)}\subset G$ of the fibre $J^k\to J^{k-1}$ must factorize via the group of translations of the fibre itself.
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