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Cone bumps: for every point of a Cauchy level there is a smooth bump with past timelike gradient on its positive region below that level

Statement

Assume Countable Choice and Dependent Choice (The Axiom of Countable Choice (ACω), The axiom of dependent choice: a relation in which every element is related to something admits an N-indexed chain) for the actual volume-time and causal suppliers. Let (M,g,N) be a globally hyperbolic time-oriented smooth Lorentzian four-manifold (Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model, Chronology, causality, strong causality, global hyperbolicity and time functions clause (c)), let t be the volume time function of The Geroch volume function: a continuous strictly increasing time function whose levels are Cauchy sets with Cauchy levels Sc=t−1(c), and let a<b be real numbers. Then for every p∈Sb, every prescribed δ>0, and every open neighborhood O of p, there exist

(a) hp has compact support contained in C; in particular hp is smooth with hp=0 on {t≤a}, and 0≤hp;

(b) hp(p)=1, and {hp>1/2} is a neighborhood of p;

(c) ∇hp is past timelike at every point of {hp>0}∩J−(Sb);

(d) the nonzero-gradient locus {q:∇hp(q)≠0} meets J−(Sb) only inside {hp>0}; more precisely, {hp>0}∩J−(Sb)={f>0}∩J−(Sb) where f:C→[0,∞) is the future-branch exponential cone function on C constructed below, and on a neighborhood of every point of that set the cutoff used below is identically one.

Facts & Assumptions

Given: Countable Choice and Dependent Choice; A globally hyperbolic (M,g,N) with volume time t (The Geroch volume function: a continuous strictly increasing time function whose levels are Cauchy sets), real numbers a<b, a point p∈Sb, and an open neighborhood O of p.

[L1]

t is continuous, strictly increasing along causal relations, its levels Sc are Cauchy hence acausal sets, and I+(Sa)={t>a}, J+(Sb)={t≥b} and J−(Sb)={t≤b} with J+(x) and J−(Sb) closed; for compact K the set J+(K)∩J−(Sb) is compact (The Geroch volume function: a continuous strictly increasing time function whose levels are Cauchy sets clauses (b)-(d), Truncated causal cones J^+(K) cap J^-(S_b) over compact sets and Cauchy levels are compact, In a globally hyperbolic manifold the causal relation is closed and truncated causal cones over compact sets are compact clauses (a) and (b)).

[L2]

In a sufficiently small convex normal ball, the future timelike endpoints from its base are exactly the exponential image of the future timelike cone (Local causality in a convex normal ball: causal reachability is the exponential cone, the Lorentzian length is bounded by the displacement radius, and null endpoints force the null geodesic clause (b)). Strictly convex normal neighborhoods: every point has arbitrarily small strictly convex normal neighborhoods C; on C the exponential exp⁡q:Wq→C is a diffeomorphism for every q∈C, the unique geodesic segment in C joins any two points, and the position vector P(q,q′)=d(exp⁡q)v(v), v=exp⁡q−1(q′), is defined with gq′(P,P)=gq(v,v) (Existence of strictly convex normal neighborhoods: small coordinate balls are normal neighborhoods of each of their points clauses (a)-(c), Normal neighborhoods, convex normal sets, the position vector and the squared-displacement function, The joint exponential map: smoothness, invertible differential at the diagonal, and the small-velocity two-point inverse).

[L3]

Gauss lemma: for the smooth function Q:C→R, Q(q′):=−gq(v,v) with v=exp⁡q−1(q′), one has ∇Q=−2P(q,q′) (the gradient being that of The inverse metric, musical isomorphisms and index raising), and the causal character of P(q,q′) equals that of v (The Lorentzian Gauss lemma and the radial maximum of proper time).

[L4]

The standard flat function φ(t)=e−1/t for t>0 and zero for t≤0 is smooth and all its derivatives vanish at zero (The standard flat function, The standard flat function is smooth and flat at zero). For t>0 each derivative is a polynomial in 1/t times e−1/t, and for every nonnegative integer m, t−me−1/t→0 as t↓0. Smooth compositions and products obey the chain and product rules (The chain rule for total derivatives: D(g∘f)(a)=Dg(f(a))∘Df(a), Cr and smooth maps between smooth manifolds, Continuity of f:A→R at a point of A and on A: the ε-δ condition, its agreement with lim⁡x→cf(x)=f(c) at a limit point, and continuity at an isolated point).

[L5]

Smooth cutoffs: for every compact K and open O with K⊆O there is a smooth χ:M→[0,1] with χ=1 on a neighborhood of K and supp⁡χ⊆O; to see the neighborhood plateau from the weaker Euclidean cutoff statement, take the family of all pairs of nested chart balls with inner closed ball inside the outer ball and outer compact closure in O. Their inner open balls form an ambient open cover of K, so a finite subfamily covers K by A subspace is compact exactly when every family of open subsets of the ambient space covering it, indexed or not, has finitely many members covering it clause 2. Apply the Euclidean supplier to each inner closed ball and its outer ball, extend by zero in the chart, and call the resulting functions χi. Then χ=1−∏i(1−χi) is one on the union of the inner open balls and has compact support in O. Empty K permits χ=0; only finite selections are used (A Euclidean bump for a compact set inside an open set, Smooth partitions of unity subordinate to an open cover).

[L7]

Diameters of small chart balls: h is a smooth Riemannian metric on M and dh its Riemannian distance (The auxiliary Riemannian metric h=g+2n-flat tensor n-flat is complete after a proper-exhaustion conformal factor, and its closed bounded sets are compact clauses (b)-(d), Riemannian distance on a connected manifold); on a compact subset K of a chart the metric h is comparable with the Euclidean metric, h(v,v)≤CK∣v∣e2 for a finite constant CK depending on K (Local comparison of a riemannian metric with the euclidean metric). Fix a Euclidean chart ball Eρ0 around p and let C be the constant of the comparison on its closure; then for every 0<ρ≤ρ0 the h-diameter of the concentric ball Eρ is at most 2Cρ, because the h-length of a curve in Eρ is at most C times its Euclidean length and any two points of Eρ are joined there by a straight segment of Euclidean length at most 2ρ.

Proof

technique · direct
1.1L1L2L7givenconstruct

(A truncated cone inside a small convex normal neighborhood.) Since b>a, the point p∈Sb satisfies t(p)=b>a, so p∈I+(Sa) by [L1]. Let δ>0 be prescribed. Choose a Euclidean chart ball Eρ0 around p with compact closure in O∩I+(Sa), let C0 be the comparison constant of [L7] on its closure, and choose 0<ρ≤ρ0 with 2C0ρ<δ. By [L2] there is a sufficiently small strictly convex normal neighborhood C of p with C‾ compact and C‾⊆Eρ⊆I+(Sa); then diam⁡h(C)≤diam⁡h(Eρ)≤2C0ρ<δ by [L7]. We claim that some p′≪p satisfies J+(p′)∩J−(Sb)⊆C. Suppose not: choose a sequence pk′→p along a future timelike curve with pk′≪p and pk′∈C, and points rk∈(J+(pk′)∩J−(Sb))∖C. For each k the causal segment from pk′ to rk leaves C, so it has a first exit point qk∈∂C∩J+(pk′)∩J−(Sb). Fix r≪p with r≤pk′ for all large k (take r before the sequence on the timelike curve through p); then qk∈J+(r)∩J−(Sb), which is compact by [L1], so a subsequence qk→q∈J+(r)∩J−(Sb)∩∂C. Since pk′→p and pk′≤qk, closedness of the causal relation [L1] gives p≤q. Also q∈J−(Sb) gives some z∈Sb with q≤z. Monotonicity of t [L1] gives b=t(p)≤t(q)≤t(z)=b, so t(q)=b, that is, q∈Sb; acausality of Sb [L1] then forces q=z, and p≤q with p,q∈Sb likewise forces q=p. Hence p=q∈∂C, contradicting p∈C with C open. This proves the claim.

1.2L2L3L4givenconstruct

(The future-branch cone function.) On C let v(q′)=exp⁡p′−1(q′) and Q(q′)=−gp′(v(q′),v(q′)), smooth by [L2]. Fix a future unit tangent n at p′ and set a(q′)=−gp′(v(q′),n). Define f:C→[0,∞) by f(q′)=φ(Q(q′)) when a(q′)>0, and f(q′)=0 when a(q′)≤0. The set {Q>0,a>0} is exactly IC+(p′) by [L2], so f>0 exactly there and f(p)>0. At any nonvertex point with a=0, the rest-space positivity gives Q<0 and f is locally zero. Elsewhere smoothness follows from composition and flatness across Q=0. At the vertex, derivatives of φ(Q) are polynomially bounded factors times flat derivatives, tending to zero faster than any power of the inverse-vector norm; the zero extension across the separating hyperplane is therefore smooth. Only smoothness on C is claimed; extension across the boundary of C will be performed after multiplication by the compact cutoff.

2.1step 1.2L3L4L6

(The gradient is past timelike.) Where f>0 one has ∇f=φ′(Q)∇Q with φ′(Q)>0 [L4], hence ∇f=−2φ′(Q) P(p′,q′) by [L3]; now q′∈I+(p′) means v is future timelike, so P(p′,q′) is future timelike with the same causal character [L2, L3], and a positive multiple of its negative is past timelike. Hence ∇f is past timelike at every point where f>0.

3.1step 1.1step 1.2step 2.1L1L5given∎

(The cutoff and the bump.) Let K=J+(p′)∩J−(Sb), a compact subset of the open set C by step 1.1 and [L1]. By [L5] choose a smooth cutoff χ:M→[0,1] with χ=1 on a neighborhood U0 of K and supp⁡χ⊆C, and define hp∣C:=χff(p),hp:=0 outside C. On C use the displayed product and define hp=0 outside C. Since supp⁡χ is compactly contained in C, this extension is smooth across the boundary of C; thus hp is a smooth function with compact support in C⊆I+(Sa)={t>a} and hp≥0; this is (a). Since p∈K⊆U0, near p one has χ=1 and hp=f/f(p), so hp(p)=1 and, by continuity, {hp>1/2} contains a neighborhood of p: this is (b). For (c): let q′∈{hp>0}∩J−(Sb). Since hp>0 forces χ>0 and f>0, we have q′∈{f>0}=IC+(p′)⊆J+(p′), so q′∈J+(p′)∩J−(Sb)=K⊆U0; on the neighborhood U0 of K the cutoff equals one, so on a neighborhood of q′ contained in U0 one has hp=f/f(p) and ∇hp=∇f/f(p), which is past timelike by step 2.1. At a point of the future null boundary or its vertex, all derivatives of f vanish; outside the future cone f is locally zero. On the cutoff plateau containing K, these facts imply that a nonzero gradient at a point of J−(Sb) forces f>0. This proves the nonzero-gradient assertion in (d). Statement (c) follows above; the remaining part of (d) is the identity {hp>0}∩J−(Sb)={f>0}∩J−(Sb) established in the same computation, together with χ=1 on U0⊇K⊇{f>0}∩J−(Sb).

Remarks

  • The point of the flat function. f is the smoothing of the indicator of the future cone: it vanishes to infinite order on the null boundary and at the vertex, which is why the composition is smooth although the cone has a corner. The exponential map converts the corner into the quadratic zero set Q=0 of a smooth function.

  • Why the cutoff is harmless. At every point of {hp>0}∩J−(Sb) the cutoff equals one on a neighborhood, so its gradient does not contribute and ∇hp is past timelike. At the future null boundary and the vertex p′ the flat cone function and its gradient vanish; no timelikeness is asserted there.

  • Use. In Weak steps: locally finite sums of cone bumps give a smooth step around each Cauchy level with past timelike gradient near the level these bumps are summed locally finitely to produce h+ with past timelike gradient on the past side, and the time-reversed construction produces the negative plateau h−.

Depends on

Dependency tree · 2 levels

Sources