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Temporal cutoff estimate for normals to maximal hypersurfaces
Statement
Let be smooth time-oriented Lorentz metrics of signature on a common smooth four-manifold, converging in to a Lorentz metric near a fixed compact set . Use a common time orientation and a fixed finite coordinate cover near , with uniformly bounded metric and inverse-metric norms. Let be a fixed smooth function, with past-directed timelike -gradient and on . Let be smooth spacelike maximal hypersurfaces, smooth up to their actual boundaries, with future unit normals , such that the entire portions are compact and contained in . Set , and when is nonempty, and when . There is , depending only on , the uniform metric and inverse bounds and in that cover, such that . A supremum over an empty set is zero. In particular the boundary supremum is retained unless it is empty or separately bounded. No uniform bound on the normals is assumed in advance.
Facts & Assumptions
Work in ZFC, including the Axiom of Choice. The Axiom of Choice
The meanings of spacelike, future normal and maximality are Spacelike sections, maximality and lapse–shift data; past timelike gradient and temporal function have the convention of Causal exterior, chronological boundaries and Cauchy data. The temporal angle, operator and compact-portion conventions are Temporal normal angle and compact positive-height portions.
The temporal gradient identity is Temporal angle and tangential height gradient identity; the conversion of a hyperbolic-angle differential inequality to the logarithmic one on is From hyperbolic angle to logarithmic angle inequalities.
The compact weighted maximum and interior exclusion lemmas are Compact weighted maximum and the actual boundary term and Differential exclusion of a large interior weighted angle maximum.
Use the exact external differential estimate in the following External input section, under the complete geometric hypotheses of the Statement.
Positive-base real powers are for and real ; the supplementary convention is for . Real powers for positive bases, with the zero-base positive-exponent convention
External input
Import (B.11) of Radu, Appendix B: with the geometric hypotheses of the Statement and , there is a uniform such that on , and . Its constant depends only on , the stated uniform coordinate metric/inverse bounds and the norm of . This is an external geometric differential estimate, not a local reconstruction. The source derives it from (B.8)–(B.10) using Gauss–Codazzi, maximality and the trace-free eigenvalue bound in three tangent dimensions; the present proof imports that step with all its hypotheses.
Proof
Given: The sequence, compact portions and temporal function in the Statement, with imported differential estimate [F4].
Goal: Prove the stated uniform weighted angle bound.
The temporal data are well defined by [F1]. If , including when , containment of the entire nonnegative-height portions in implies that the positive-height sets are empty, so the conclusion holds for any fixed by the zero-supremum convention. Otherwise put . By [F4] choose a common for both differential estimates. By [F2] its hyperbolic-angle inequality gives on , and .
Choose a common so that . The exclusion lemma [F3] rules out a local interior maximum of at positive height with . The compact maximum lemma [F3] then gives , where is exactly the actual boundary supremum in the Statement. The choice of uses only the uniform geometric constant, and , itself bounded by the specified norm. This proves the stated bound for every with all boundary terms intact.
Source notes
The scalar argument follows the maximum-principle method of Radu, Appendix B, (B.11)–(B.12), using the explicitly proved conversion to log v and retaining the source’s conservative stated constant. The independent source is not the article under study. No graph existence, temporal-function existence, boundary-angle estimate or tensor-identity reconstruction is asserted. The compact sets must contain the entire nonnegative-height portions; replacing them by intersections with an arbitrary compact Q would introduce extra boundary terms.
Depends on
- Spacelike sections, maximality and lapse–shift data
- Causal exterior, chronological boundaries and Cauchy data
- The Axiom of Choice
- Real powers for positive bases, with the zero-base positive-exponent convention
- Temporal normal angle and compact positive-height portions
- Temporal angle and tangential height gradient identity
- From hyperbolic angle to logarithmic angle inequalities
- Compact weighted maximum and the actual boundary term
- Differential exclusion of a large interior weighted angle maximum
- Alexandru F. Radu, Rigidity of stationary black holes with small ADM angular momentum, arXiv:2610.09729v1 · Appendix B, Lemma B.1 and (B.1), PDF/printed pp.35–36; proof (B.8)–(B.12), pp.38–39, especially (B.11)
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External dependencies
In a time-oriented Lorentzian four-manifold, for smooth Lorentz metrics g_j converging in C2 near a fixed compact Q, a fixed smooth τ with past timelike g_j-gradient and α_j²=-g_j^{-1}(dτ,dτ)≥a0²>0 on Q∩{τ≥0}, and smooth spacelike maximal Σ_j with future unit normals whose entire portions Σ_j∩{τ≥0} are compact and contained in Q, put V_j=-α_j^{-1}grad_{g_j}τ and v_j=-g_j(n_j,V_j). There is a uniform C such that, on {v_j>2}, η_j=arcosh v_j satisfies Δ_{Σ_j}η_j≥cothη_j(¼|∇_{Σ_j}η_j|²-Cv_j²) and |Δ_{Σ_j}τ|≤Cv_j². The constant is controlled by a0, the uniform coordinate C2 metric/C0 inverse bounds and the coordinate C3 norm of τ. Lemma B.1 concludes sup τ^μ v_j≤2 max{2τmax^μ,sup_{∂Σ_j∩{τ>0}}τ^μ v_j} for some μ>4 controlled by the same geometry. The empty boundary supremum is zero.
Hypotheses: Common time orientation, signature (-,+,+,+), spacetime dimension four; fixed finite coordinate cover near Q; uniform C2 bounds for g_j, C0 bounds for inverses, and C3 bounds for fixed τ; past timelike gradient with the stated lower norm bound; smooth spacelike maximal hypersurfaces and future unit normals, smooth up to their actual boundaries; entire nonnegative-height portions compact and contained in Q. No vacuum or field equation, stationary-graph representation, or boundary-angle bound is presumed; actual boundary terms are retained.
Reading limits: Read the v1 PDF text of Lemma B.1 and (B.1) on printed/PDF pp.35–36 and its proof (B.8)–(B.12) on pp.38–39 through web PDF retrieval during this repair. Checked the imported inequalities, geometric hypotheses, constant dependence and actual-boundary term against those passages. Page-image retrieval was unavailable. The tensor/coefficient estimates leading to (B.11) are imported established input and were not independently reconstructed. The local conversion and maximum lemmas and their application below supply the locally composed argument; they do not reconstruct those tensor estimates.
Sources
- Alexandru F. Radu, Rigidity of stationary black holes with small ADM angular momentum, arXiv:2610.09729v1 · Appendix B, Lemma B.1 and (B.1), PDF/printed pp.35–36; proof (B.8)–(B.12), pp.38–39, especially (B.11)