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Nonlinear stability of subextremal Kerr black holes

Peter Hintz

Jun 26, 2026arXiv:2606.28253v1
gr-qcmath.AP
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Scorecard· 5/16
10.0/10 impact

Abstract

We settle the global nonlinear stability problem for the family of Kerr black holes in the full subextremal range: spacetimes evolving from initial data close to those of a subextremal Kerr black hole as solutions of the Einstein vacuum equation Ric(g)=0{\rm Ric}(g)=0 settle down to a nearby member of the Kerr family at the rate O(t2εK)\mathcal{O}(t_*^{-2-ε_{\mathcal K}}) in spatially compact regions. For the initial data, we require O(r1ε0)\mathcal{O}(r^{-1-ε_0})-decay for ε0>0ε_0>0 -- more precisely, an arbitrary but finite expansion into terms rz(logr)kr^{-z}(\log r)^k where z>1z>1, kN0k\in\mathbb{N}_0, plus a remainder term with O(r3ε0)\mathcal{O}(r^{-3-ε_0})-decay. Similarly to previous work with Vasy in the Kerr-de Sitter setting, we use a generalized wave map gauge modified using gauge source terms that lie in a suitable finite-dimensional space determined by the expansion of the initial data. Like the final black hole parameters (mass and angular momentum) and the gravitational wave tail, the gauge source terms are treated as unknowns in a nonlinear (Nash-Moser) iteration scheme. We work directly with the tensorial equation and in particular do not rely on reductions to scalar equations (except insofar as a reduction to the Teukolsky equation is used in the proof of linear mode stability). This paper relies on two companion papers by the author. The first one introduces a strong form of constraint damping in the full subextremal range, which we use in our formulation of the gauge-fixed Einstein equation as a black box. The second one provides tame estimates (albeit with weak decay) for forward solutions of a general class of wave-type equations, which we show here to include the linearizations of the gauge-fixed Einstein equation arising in our nonlinear iteration scheme; these estimates are the starting point for our detailed asymptotic analysis.

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Scientific Impact Assessment: "Nonlinear stability of subextremal Kerr black holes" by Peter Hintz

1. Core Contribution

This paper resolves one of the most celebrated open problems in mathematical general relativity: the global nonlinear stability of the Kerr family of black holes in the full subextremal range |a| < m. The main result (Theorem 1.1) establishes that spacetimes evolving from initial data close to subextremal Kerr settle down to a nearby Kerr black hole at rate O(t⁻²⁻ᵋ) in spatially compact regions. This extends previous results that were restricted to slowly rotating (|a₀| ≪ m₀) or axially symmetric settings.

The paper introduces a comprehensive framework for analyzing quasilinear wave equations on asymptotically flat spacetimes, centered on several key innovations:

  • Generalized wave map gauge with finite-dimensional gauge source terms: The gauge issues in the Kerr stability problem are shown to be finite-dimensional in nature, with gauge source terms treated as unknowns in a Nash-Moser iteration.
  • A systematic framework for wave decay on asymptotically flat spacetimes: The paper develops a unified picture (Figure 1.3) explaining how decay and asymptotics propagate across four asymptotic regimes (spatial infinity, null infinity, future timelike infinity, and the Kerr face).
  • Direct tensorial approach: Unlike many prior works, the analysis works directly with the tensorial Einstein equation without reducing to scalar equations (except for mode stability via the Teukolsky equation).
  • 2. Methodological Rigor

    The paper demonstrates extraordinary methodological sophistication across 329 pages:

  • Microlocal and spectral analysis: The proof relies on b-analysis, scattering-b-transition analysis, and 3b-analysis frameworks, rigorously controlling regularity and decay in all asymptotic regimes simultaneously.
  • Nash-Moser iteration: The nonlinear problem is solved via a carefully designed iteration scheme where linearized problems are solved globally with precise tame estimates, tracking regularity loss through ~O(d) derivatives per step.
  • Companion papers: The paper builds on two companion works—one on constraint damping [Hin26a] providing "enhanced mode stability" at zero energy (widening the indicial gap), and another [Hin26b] providing tame estimates for wave-type equations on asymptotically flat spacetimes.
  • Partial polyhomogeneity: The paper carefully tracks asymptotic expansions with controlled index sets at all boundary hypersurfaces, a technically demanding but essential ingredient.
  • The verification of every hypothesis from the general framework for the specific case of linearized Einstein equations (mode stability, trapping admissibility, tf-admissibility, 2-admissibility) is thorough and complete.

    3. Potential Impact

    Within mathematical GR: This settles the Kerr stability conjecture and opens several directions:

  • Unconditional C⁰-stability of the Cauchy horizon (via Dafermos-Luk)
  • Smooth dynamical event horizons (via Chen-Klainerman and the author's prior work)
  • Construction of black hole merger spacetimes
  • The framework likely extends to Einstein-Maxwell (Kerr-Newman) and other coupled systems
  • For PDE theory: The systematic framework for wave asymptotics on asymptotically flat spacetimes, the treatment of the transition between different asymptotic regimes via normal operator families, and the efficient parameterization of solutions via ι⁺-asymptotics (§12) represent substantial advances in microlocal analysis applicable beyond GR.

    For numerical relativity: The constraint damping strategy and the precise gauge conditions developed here inform numerical implementations.

    4. Timeliness & Relevance

    This paper arrives at a moment of intense activity: partial results by Klainerman-Szeftel (slowly rotating), Dafermos-Holzegel-Rodnianski-Taylor (Schwarzschild), and others had made significant progress. The full subextremal result was widely considered the key remaining challenge. The paper also establishes t⁻³ decay (Remark 1.2, §13.2), improving on the t⁻¹⁻ᵋ rates of previous works—this is significant for understanding gravitational wave tails.

    5. Strengths & Limitations

    Key strengths:

  • Completeness: handles the full subextremal range without symmetry assumptions
  • The O(r⁻¹⁻ᵋ₀) initial data assumptions are physically reasonable, allowing partial polyhomogeneity
  • The t⁻³ decay rate is essentially sharp (bounded below by Price's law contributions from physical modes h⁽⁻²⁾_{b,s2/v2})
  • The framework produces three immediate corollaries (Cauchy horizon stability, event horizon regularity, merger spacetimes)
  • Self-contained treatment of spectral theory at all energy scales
  • Notable limitations:

  • The extremal case |a| = m remains open (and is expected to be unstable)
  • Initial data must decay as O(r⁻¹⁻ᵋ₀), slightly faster than the O(r⁻¹) suggested by physically motivated constructions of Kehrberger-Kadar
  • The paper length (329 pages plus two companion papers) makes complete verification challenging
  • Removing partial polyhomogeneity in favor of "structureless" O(r⁻¹⁻δ) decay is described as a technical but open problem
  • Additional observations:

  • The paper includes a compelling Conjecture 13.8 on Bondi mass, connecting the boost parameter to initial/final mass comparison
  • The efficient parameterization in §12 is a conceptual innovation that cleanly separates the formal asymptotic construction from the forward problem
  • Smooth dependence on parameters (including across the Schwarzschild limit a=0, where the cokernel structure changes) is handled with care
  • This paper represents a monumental achievement in mathematical physics, resolving a problem that has driven development in geometric analysis and PDE theory for decades.

    Rating:10/ 10
    Significance 10Rigor 9.5Novelty 9.5Clarity 8.5

    Generated Jun 29, 2026

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