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Controlled horizon cuts, compact restrictions and a uniform end anchor

Statement

Work in ZFC. Let X‾ be a connected smooth three-manifold with compact boundary S, with specified smooth inner collar [0,r0)×S and a disjoint Cartesian end E={x∈R3:∣x∣>R0}. Require that X‾∖{∣x∣>R} is compact for every sufficiently large R. Put X=X‾∖S. Supply a stationary product M=Rt×X: each smooth time-oriented Lorentz metric gq has signature (−,+,+,+), and the translations (t,z)↦(t+c,z) are time-orientation-preserving isometries, with T=∂t. Let Q⊆(0,1] index smooth spacelike graphs Γq={(uq(z),z):z∈X}, with future unit normals nq and positive lapses Nq=−gq(T,nq). Thus the candidates are supplied over the entire base, including the region between the two collars.

In the common complete boost/circle collar write (r,η,y), K=∂η, T=∂η−ΩZS, with κ>0 and compact sphere S. The reference section t=0 is η=a(r,y), ∣a∣≤A, satisfying the reference transversality and timelike-K hypotheses of the bounded-rapidity and complete-reference-product results. Its r coordinate agrees with the supplied base collar. Assume the candidates in this collar are also rapidity graphs η=a(r,y)+bq(r,y), ∣bq∣≤B. In a fixed open physical neighborhood U of S, suppose their unit normals have uniformly bounded components in fixed smooth ambient frames. The complete collar agrees near S with its normal exponential tube.

For a common sufficiently small ε>0, all candidate cuts over r=ε lie in U and inherit its normal bounds. They are stationary-base level cuts. For any sufficiently large fixed R, these inner cuts and the end cuts over ∣x∣=R bound compact smooth graph restrictions over the same connected compact smooth domain Ωε,R⊂X, whose boundary is exactly those two base cuts. Any prescribed compact target in X can be included in its interior. A separate common bound ∣uq∣≤H on this fixed domain encloses the restrictions in the fixed compact tube [−H,H]×Ωε,R.

For the end assertion supply constants dq≥1 and define cq=dq/(4q), tq=cqt, xq=qx, and u~q(xq)=cquq(xq/q). Assume the component matrices of gq in (tq,xq) converge uniformly to diag⁡(−1,1,1,1), and ∣Dxqu~q∣→0 uniformly, as ∣xq∣→∞, with a common threshold over the parameter set in question. On this common normalized end put Fq=tq−u~q(xq) and sq=−gq−1(dFq,dFq). There is a common ρ∗>R0 such that Nq=cq/sq≥1/8 and the normalized coordinate components of nq are bounded wherever ∣xq∣≥ρ∗. Thus a fixed normalized spatial point ξ with ∣ξ∣≥ρ∗ is an anchor over the original base point x=ξ/q. For each fixed δ∈(0,1], a fixed original base point with δ∣x∗∣≥ρ∗ is an anchor simultaneously for q∈Q∩[δ,1]; original coordinate normal components are uniformly bounded on a fixed sufficiently distant end cut for this subfamily. One may choose the outer cut beyond x∗ so that the anchor lies inside the restrictions. The same conclusions apply when the uniform end hypotheses are supplied only on this positive-parameter subfamily. A fixed original base point is not asserted uniformly as q↓0.

The conclusions also hold for an arbitrary indexed collection (qi,Γi)i∈I, with qi∈(0,1] and a supplied global graph Γi={(ui(z),z):z∈X} for gqi. Impose the same positive-lapse, collar and uniform normalized-end hypotheses over these indices, including η=a+bi with ∣bi∣≤B, the common physical-neighborhood normal bound, and uniform normalized slope decay for u~i(xqi)=cqiui(xqi/qi). The compact-tube conclusion retains the independent common bound ∣ui∣≤H on the fixed cut domain. Distinct indices may have the same parameter and different graphs. The cuts and normalized-end threshold are common over the indexed collection. On Iδ={i:qi≥δ} the original-base anchor and original-coordinate normal bounds are common as above, also when the uniform end hypotheses are supplied only on this subcollection.

Facts & Assumptions

[A1]

Work under the Axiom of Choice, including the inherited choice hypotheses of the stationary-level and normal-coordinate suppliers. The Axiom of Choice

[F1]

The normal exponential tube has Ξ(y,v0,v1)=exp⁡y(v0e0+v1e1) with v0=rsinh⁡(κη) and v1=rcosh⁡(κη). The bounded reference rapidity gives ∣t−η∣≤A in the complete collar, whose complete reference flow and agreement with the physical tube are the supplied collar model. Circle-invariant normal coordinates linearize a bifurcate Killing boost A smooth spacelike reference section is a bounded rapidity graph A complete timelike collar flow is a reference product

[F2]

The product smooth structure is the canonical one. The supplied spacelike graphs, unit normals and lapses use the stated hypersurface conventions. A smooth stationary graph with positive lapse restricts over every compact smooth base domain to a compact spacelike hypersurface with its actual graph boundaries, and a common height bound gives a compact stationary tube. Products of smooth manifolds have a canonical product smooth structure Spacelike sections, maximality and lapse–shift data Positive-lapse stationary graphs give temporal level functions and closed restrictions

[F3]

Smooth domains carry their manifold-with-boundary smooth structures and smooth inclusions. A closed subspace of a compact space is compact, and a continuous image of a connected space is connected. Closed bounded intervals and finite products of compact spaces are compact. An open neighborhood of a compact factor times a point contains a product neighborhood. Embedded smooth submanifolds with boundary A closed subspace of a compact space is compact, and a finite union of compact subspaces is compact A continuous image of a connected space is connected, and connectedness is a topological property Heine-Borel by bisection: every closed bounded interval [a,b] is compact A product of finitely many compact spaces is compact in the product topology Tube lemma: if K is compact and an open N ⊆ X × Z contains K × {z₀}, then N contains K × W for some open W ∋ z₀

[F4]

The inverse metric and the musical map identify grad⁡gqFq with gq−1dFq in coordinates. This supplier has domain mathematics. The rescalings, uniform matrix convergence and normalized slopes above are explicit local data, not a Harrison or field-equation input. The inverse metric, musical isomorphisms and index raising

Proof

Given: The supplied global stationary graphs, compact-core end geometry, complete physical collar, controlled collar normals and explicit uniform normalized end hypotheses. Goal: Construct common controlled restrictions and locate the uniform end anchors in the stated coordinates and parameter ranges.

1.1A1F1F2F3givenchoose

On every candidate collar cut, ∣η∣≤A+B. Set L=A+B. The compact set S×[−L,L] and the normal-tube map in [F1] give a continuous map (y,η,r)↦Ξ(y,rsinh⁡(κη),rcosh⁡(κη)), defined for small r≥0 and equal to y∈S at r=0. Compactness of the interval and product and the tube lemma [F3], applied to the inverse image of U intersected with the physical tube, give one ε0>0 for all y,η. Thus every 0<ε<ε0 places the cuts in U, and their normal bounds are inherited. Since T(r)=0, these are fixed stationary-base cuts. The comparison in [F1] also gives ∣t∣≤2A+B on them.

1.2F3givenconstruct

Delete the open inner subcollar 0≤r<ε and the open end tail ∣x∣>R from X‾, obtaining Ωε,R. It is a closed subspace of the supplied compact set X‾∖{∣x∣>R}, hence compact by [F3]. Near its inner cut the coordinate r−ε≥0 is a smooth boundary coordinate, and near its outer cut R−∣x∣≥0 is one; the cuts are disjoint and all other points have interior charts. These charts give the embedded codimension-zero smooth structure in [F3], with boundary exactly the two cuts. Clamping r to max⁡(r,ε) in the inner collar and the end radius to min⁡(∣x∣,R), leaving all other points fixed, defines a continuous retraction of connected X‾ onto this domain. The formulas agree with the identity near the collar interfaces, so [F3] makes the image connected. The interiors of such domains exhaust X as ε decreases and R increases. Their open cover of any fixed compact target has a finite subcover, so one sufficiently small ε and large R include the target in the interior.

1.3F2F4givenalgebra

In normalized components write Gq for the metric matrix and m=diag⁡(−1,1,1,1). Uniform Gq→m implies uniform Gq−1→m: the entries of the inverse are adjugate entries divided by determinant, which tends to det⁡m=−1 and hence is uniformly separated from zero on a common end. The covector components of dFq are (1,−Du~q), tending uniformly to (1,0,0,0). Therefore sq2→1 uniformly. Increase a common ρ∗>R0 until 1/2≤sq≤2 and the inverse components are bounded for ∣xq∣≥ρ∗. The future normal is nq=−grad⁡gqFq/sq, by the positive-lapse level-function identity in [F2], unchanged under the positive rescaling Fq=cq(t−uq). Its normalized components are bounded by [F4] and these estimates. Since dFq(T)=cq, Nq=−gq(T,nq)=cq/sq≥1/8, using dq≥1 and q≤1.

2.1F2step 1.1step 1.2given

Every uq is supplied smooth on all of X, not only the collar. Thus [F2] applies to the fixed domain from step 1.2 and each stationary metric and positive-lapse graph: its restriction is compact smooth spacelike, with manifold boundary exactly the graphs over both cuts. The independent hypothesis ∣uq∣≤H on this domain then gives the common compact tube by [F2]. No global graph or middle-region height bound has been inferred from collar control.

3.1F2F4step 1.2step 2.1step 1.3givenalgebra

A fixed normalized spatial point ξ beyond ρ∗ corresponds exactly to x=ξ/q, so step 1.3 gives the all-parameter normalized anchor. On q∈Q∩[δ,1], every fixed original point with δ∣x∗∣≥ρ∗ satisfies ∣qx∗∣≥ρ∗, giving a common original-base anchor. Its candidate point is (uq(x∗),x∗); extending normal and lapse by stationary translation as in [F2] evaluates the same lapse at the fixed ambient point (0,x∗). For vector components the conversion is nqt=cq−1nqtq and nqxi=q−1nqxqi. Here cq−1=4q/dq≤4 and q−1≤δ−1, so step 1.3 also bounds original normal components on any fixed end cut with δR≥ρ∗. Choose R>∣x∗∣ in step 1.2 to retain the anchor inside the restrictions. These arguments can be applied to a subfamily with its own common normalized threshold. They assert no fixed original anchor when q has no positive lower bound.

4.1F2F4step 1.1step 1.2step 1.3step 2.1step 3.1givenalgebra∎

For the indexed collection, repeat step 1.1 with bi: its compact set S×[−A−B,A+B] and fixed normal-tube map are independent of the index, so the same ε0 works for every graph. The domain constructed in step 1.2 depends only on the base and the two cut radii. Apply step 2.1 separately to each supplied global graph; its positive lapse and the independent common height bound give the same compact tube. For the end calculation in step 1.3 use the metric matrix at qi and the conormal of Γi. Uniform metric convergence and slope decay over the indexed collection imply one common threshold with 1/2≤si≤2. The identical conormal normalization gives Ni=cqi/si≥1/8 and bounded normalized normal components. On Iδ the inequalities ∣qix∗∣≥δ∣x∗∣, cqi−1≤4 and qi−1≤δ−1 give the same common original-base anchor and coordinate bounds as step 3.1. If end uniformity is supplied only on that subcollection, perform precisely this end calculation there with its common threshold. None of these constructions selects a unique graph for a parameter; all constants use the stated common data. Thus they apply simultaneously when parameters repeat with distinct supplied graphs.

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