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arXiv 2608.10518math.DGmath.AP

无穷远曲率决定具有有限指标薛定谔算子的完备非紧曲面的拓扑

Curvature at Infinity Governs the Topology of Complete Non-Compact Surfaces Admitting Schrödinger Operators of Finite Index

Hideaki Harumoto, Kei Kondo

AI总结:

该研究探究容许有限指标薛定谔算子的完备非紧黎曼曲面,证明其无穷远曲率决定整体拓扑与几何刚性,推导相关恒等式、端点数界,明确两种几何视角下的控制机制。

AI中文摘要:

本文研究了容许带有非负位势且具有有限 Morse 指标的薛定谔算子的完备非紧黎曼 2 维流形 Σ 的整体拓扑。Fischer-Colbrie 的经典结果在指标消失或几何稳定性的假设下,将这类流形分类为黎曼 3 维流形中的浸入极小曲面;我们证明,无需施加上述任一假设,由 Fischer-Colbrie 定理给出的正函数确定的完备共形度量 g^* 的无穷远曲率 λ_∞^*(Σ) 决定了 Σ 的整体拓扑与几何刚性。更确切地说,我们推导了一个将 λ_∞^*(Σ) 与 (Σ,g^*) 的面积增长相关联的基本恒等式,证明了来自固定基点 p 的距离函数 d_p^* 的所有临界点都被限制在一个有界区域内,并作为推论得到了端点数的定量界。我们进一步区分了两种互补的几何视角:一方面,λ_∞^*(Σ) 的一个定量条件迫使 Σ 微分同胚于欧几里得平面 ℝ²;另一方面,当 Σ 恰好有一个端时,λ_∞^*(Σ) 的另一个条件保证了 (Σ,g^*) 上的每一个 Busemann 函数都是耗尽函数。通过阐明这两种机制(相对于基点的距离函数的临界点结构与无穷远 Busemann 函数的整体行为)之间的关系,我们展示了 λ_∞^*(Σ) 控制 Σ 的整体几何与拓扑的两种互补表现形式。

英文摘要:

In this article, we investigate the global topology of a complete non-compact Riemannian $2$-manifold $Σ$ admitting a Schrödinger operator with non-negative potential and finite Morse index. While classical results of Fischer-Colbrie classify such manifolds under the assumption of vanishing index or geometric stability as immersed minimal surfaces in a Riemannian $3$-manifold, we show that the curvature at infinity $λ_\infty^*(Σ)$ of the Fischer-Colbrie metric $g^*$---a complete conformal metric determined by a positive function furnished by Fischer-Colbrie's theorem---governs the global topology and geometric rigidity of $Σ$ without imposing either assumption. More precisely, we derive a fundamental identity relating $λ_\infty^*(Σ)$ to the area growth of $(Σ,g^*)$, show that all critical points of the distance function $d_p^*$ from a fixed base point $p$ are confined to a bounded region, and, as a corollary, obtain a quantitative bound for the number of ends. We further distinguish two complementary geometric viewpoints. On the one hand, a quantitative condition on $λ_\infty^*(Σ)$ forces $Σ$ to be diffeomorphic to the Euclidean plane $\mathbb{R}^2$. On the other hand, when $Σ$ has exactly one end, another condition on $λ_\infty^*(Σ)$ guarantees that every Busemann function on $(Σ,g^*)$ is an exhaustion. By clarifying the relationship between these two regimes---the critical-point structure of distance functions relative to a base point and the global behavior of Busemann functions at infinity---we exhibit two complementary manifestations of how $λ_\infty^*(Σ)$ controls the global geometry and topology of $Σ$.

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