黎曼流形的平面波极限

Amir Babak Aazami
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引用次数: 0

摘要

利用布劳等人对彭罗斯平面波极限的协变表述,我们为任何黎曼度量$g$构建了一个高维度的 "平面波极限 "族。这些极限沿 g$ 的测地线取值,得到洛伦兹特征的简化度量,并且是等距不变式。我们还可以看到,它们是由$g$在费米坐标中的适当展开局部产生的,它们直接编码了$g$的大部分几何。例如,$g$ 的法雅各比场被编码为其平面波极限的测地线。此外,如果且只有当其每个平面波极限都是局部保角平坦时,$g$ 才会具有恒定的截面曲率。事实上,只有当$g$的所有平面波极限都相同时,它才是平坦的,或里奇平的,或大地完全的。在极限中还保留了许多其他曲率性质,包括某些不等式,例如带符号的里奇曲率。
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Plane wave limits of Riemannian manifolds
Utilizing the covariant formulation of Penrose's plane wave limit by Blau et al., we construct for any Riemannian metric $g$ a family of "plane wave limits" of one higher dimension. These limits are taken along geodesics of $g$, yield simpler metrics of Lorentzian signature, and are isometric invariants. They can also be seen to arise locally from a suitable expansion of $g$ in Fermi coordinates, and they directly encode much of $g$'s geometry. For example, normal Jacobi fields of $g$ are encoded as geodesics of its plane wave limits. Furthermore, $g$ will have constant sectional curvature if and only if each of its plane wave limits is locally conformally flat. In fact $g$ will be flat, or Ricci-flat, or geodesically complete, if and only if all of its plane wave limits are, respectively, the same. Many other curvature properties are preserved in the limit, including certain inequalities, such as signed Ricci curvature.
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