Table of Contents
Fetching ...

Computer-assisted construction of $SU(2)$-invariant negative Einstein metrics

Qiu Shi Wang

TL;DR

The paper proves the existence of a 2-parameter family of complete negative Einstein metrics that are $SU(2)$-invariant and cohomogeneity-one on the complex line bundle $\mathcal{O}(-4)$, with metrics that are conformally compact and asymptotically hyperbolic yet generally non-Kähler and non-self-dual. The authors combine a local singular-orbit analysis, a fixed-point argument for a nearby true solution, and a global infinity extension via a conformally compact reformulation, all supported by rigorous computer-assisted numerics using Chebyshev approximations and interval arithmetic. The method builds on and extends ideas from Buttsworth–Hodgkinson, providing a robust, reproducible pipeline to certify new triaxial Einstein metrics and suggesting applicability to other cohomogeneity-one curvature problems. The results contribute explicit examples of nontrivial negative Einstein geometries with controlled asymptotics, enriching the landscape of known Bianchi IX solutions and offering a practical framework for future computer-assisted geometric analysis.

Abstract

We construct a 2-parameter family of new triaxial $SU(2)$-invariant complete negative Einstein metrics on the complex line bundle $\mathcal{O}(-4)$ over $\mathbb{C}P^1$. The metrics are conformally compact and generically neither Kähler nor self-dual. The proof involves using rigorous numerics to produce an approximate Einstein metric to high precision in a bounded region containing the singular orbit or "bolt", which is then perturbed to a genuine Einstein metric using fixed-point methods. At the boundary of this region, the latter metric is sufficiently close to hyperbolic space for us to show that it indeed extends to a complete, asymptotically hyperbolic Einstein metric.

Computer-assisted construction of $SU(2)$-invariant negative Einstein metrics

TL;DR

The paper proves the existence of a 2-parameter family of complete negative Einstein metrics that are -invariant and cohomogeneity-one on the complex line bundle , with metrics that are conformally compact and asymptotically hyperbolic yet generally non-Kähler and non-self-dual. The authors combine a local singular-orbit analysis, a fixed-point argument for a nearby true solution, and a global infinity extension via a conformally compact reformulation, all supported by rigorous computer-assisted numerics using Chebyshev approximations and interval arithmetic. The method builds on and extends ideas from Buttsworth–Hodgkinson, providing a robust, reproducible pipeline to certify new triaxial Einstein metrics and suggesting applicability to other cohomogeneity-one curvature problems. The results contribute explicit examples of nontrivial negative Einstein geometries with controlled asymptotics, enriching the landscape of known Bianchi IX solutions and offering a practical framework for future computer-assisted geometric analysis.

Abstract

We construct a 2-parameter family of new triaxial -invariant complete negative Einstein metrics on the complex line bundle over . The metrics are conformally compact and generically neither Kähler nor self-dual. The proof involves using rigorous numerics to produce an approximate Einstein metric to high precision in a bounded region containing the singular orbit or "bolt", which is then perturbed to a genuine Einstein metric using fixed-point methods. At the boundary of this region, the latter metric is sufficiently close to hyperbolic space for us to show that it indeed extends to a complete, asymptotically hyperbolic Einstein metric.
Paper Structure (32 sections, 9 theorems, 165 equations, 2 figures, 3 tables)

This paper contains 32 sections, 9 theorems, 165 equations, 2 figures, 3 tables.

Key Result

Theorem 3.1

For $t\in[a,b]$, if $\beta\geq 0$ and $u$ satisfies then

Figures (2)

  • Figure 1: Numerical evidence for the existence of complete negative Einstein metrics in the parameter plane $(h,b_1)$ for an $\dot a(0)=2$ bolt, corresponding to the total space $M=\mathcal{O}(-4)$. The dark shaded region corresponds to likely complete Einstein metrics. The region with negative $b_1$ is not shown, as there is a symmetry $b_1\leftrightarrow -b_1$, $b\leftrightarrow c$.
  • Figure 2: Plot of the warping functions of the Einstein metric constructed in § \ref{['computersection']}, with $h=1.5$, $b_1=0.1$. The cutoff time where the fixed-point construction of §\ref{['fixedpointsection']} meets the asymptotic hyperbolicity estimates of §\ref{['infinitysection']} is indicated by the brown dashed line. The numerics are produced using an order 8 Runge--Kutta solver.

Theorems & Definitions (11)

  • Theorem 3.1
  • Lemma 3.2
  • proof
  • Lemma 5.1
  • proof
  • Lemma 5.2
  • Lemma 5.3
  • Theorem 5.4
  • Lemma 5.5
  • Theorem 6.1
  • ...and 1 more