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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 (), The axiom of dependent choice: a relation in which every element is related to something admits an -indexed chain) for the actual volume-time and causal suppliers. Let 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 be the volume time function of The Geroch volume function: a continuous strictly increasing time function whose levels are Cauchy sets with Cauchy levels , and let be real numbers. Then for every , every prescribed , and every open neighborhood of , there exist
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a point with and for some strictly convex normal neighborhood of with compact, and , where denotes the auxiliary complete Riemannian metric of 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 and its Riemannian diameter (Riemannian distance on a connected manifold), and
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a smooth function such that
(a) has compact support contained in ; in particular is smooth with on , and ;
(b) , and is a neighborhood of ;
(c) is past timelike at every point of ;
(d) the nonzero-gradient locus meets only inside ; more precisely, where is the future-branch exponential cone function on 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 with volume time (The Geroch volume function: a continuous strictly increasing time function whose levels are Cauchy sets), real numbers , a point , and an open neighborhood of .
is continuous, strictly increasing along causal relations, its levels are Cauchy hence acausal sets, and , and with and closed; for compact the set 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)).
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 ; on the exponential is a diffeomorphism for every , the unique geodesic segment in joins any two points, and the position vector , , is defined with (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).
Gauss lemma: for the smooth function , with , one has (the gradient being that of The inverse metric, musical isomorphisms and index raising), and the causal character of equals that of (The Lorentzian Gauss lemma and the radial maximum of proper time).
The standard flat function for and zero for is smooth and all its derivatives vanish at zero (The standard flat function, The standard flat function is smooth and flat at zero). For each derivative is a polynomial in times , and for every nonnegative integer , as . Smooth compositions and products obey the chain and product rules (The chain rule for total derivatives: , and smooth maps between smooth manifolds, Continuity of at a point of and on : the - condition, its agreement with at a limit point, and continuity at an isolated point).
Smooth cutoffs: for every compact and open with there is a smooth with on a neighborhood of and ; 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 . Their inner open balls form an ambient open cover of , so a finite subfamily covers 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 . Then is one on the union of the inner open balls and has compact support in . Empty permits ; 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).
Timelike and causal displacement: implies ; the future timelike cone in each tangent space is open and convex and its closure contains the future causal cone; a smooth curve with future timelike velocity everywhere is a future timelike curve (The timelike set has exactly two convex components, described in orthonormal coordinates, Timelike, null, spacelike and causal vectors of a Lorentz vector space, Observers, rest spaces and the spatial projection at an event, The geodesic initial-value problem and the exponential map of the metric-selected connection, Covariant differentiation along curves: metric pairing, parallel transport and geodesic speed clause 3, Chart independence, concatenation, reparametrization and transitivity for causal curves clause (c)).
Diameters of small chart balls: is a smooth Riemannian metric on and 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 of a chart the metric is comparable with the Euclidean metric, for a finite constant depending on (Local comparison of a riemannian metric with the euclidean metric). Fix a Euclidean chart ball around and let be the constant of the comparison on its closure; then for every the -diameter of the concentric ball is at most , because the -length of a curve in is at most times its Euclidean length and any two points of are joined there by a straight segment of Euclidean length at most .
Proof
(A truncated cone inside a small convex normal neighborhood.) Since , the point satisfies , so by [L1]. Let be prescribed. Choose a Euclidean chart ball around with compact closure in , let be the comparison constant of [L7] on its closure, and choose with . By [L2] there is a sufficiently small strictly convex normal neighborhood of with compact and ; then by [L7]. We claim that some satisfies . Suppose not: choose a sequence along a future timelike curve with and , and points . For each the causal segment from to leaves , so it has a first exit point . Fix with for all large (take before the sequence on the timelike curve through ); then , which is compact by [L1], so a subsequence . Since and , closedness of the causal relation [L1] gives . Also gives some with . Monotonicity of [L1] gives , so , that is, ; acausality of [L1] then forces , and with likewise forces . Hence , contradicting with open. This proves the claim.
(The future-branch cone function.) On let and , smooth by [L2]. Fix a future unit tangent at and set . Define by when , and when . The set is exactly by [L2], so exactly there and . At any nonvertex point with , the rest-space positivity gives and f is locally zero. Elsewhere smoothness follows from composition and flatness across . At the vertex, derivatives of 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 is claimed; extension across the boundary of will be performed after multiplication by the compact cutoff.
(The gradient is past timelike.) Where one has with [L4], hence by [L3]; now means is future timelike, so is future timelike with the same causal character [L2, L3], and a positive multiple of its negative is past timelike. Hence is past timelike at every point where .
(The cutoff and the bump.) Let , a compact subset of the open set by step 1.1 and [L1]. By [L5] choose a smooth cutoff with on a neighborhood of and , and define On use the displayed product and define outside . Since is compactly contained in , this extension is smooth across the boundary of ; thus is a smooth function with compact support in and ; this is (a). Since , near one has and , so and, by continuity, contains a neighborhood of : this is (b). For (c): let . Since forces and , we have , so ; on the neighborhood of the cutoff equals one, so on a neighborhood of contained in one has and , 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 forces f>0. This proves the nonzero-gradient assertion in (d). Statement (c) follows above; the remaining part of (d) is the identity established in the same computation, together with on .
Remarks
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The point of the flat function. 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 of a smooth function.
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Why the cutoff is harmless. At every point of the cutoff equals one on a neighborhood, so its gradient does not contribute and is past timelike. At the future null boundary and the vertex the flat cone function and its gradient vanish; no timelikeness is asserted there.
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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 with past timelike gradient on the past side, and the time-reversed construction produces the negative plateau .
Depends on
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
The axiom of dependent choice: a relation in which every element is related to something admits an -indexed chain
The Geroch volume function: a continuous strictly increasing time function whose levels are Cauchy sets
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
Chronology, causality, strong causality, global hyperbolicity and time functions
Existence of strictly convex normal neighborhoods: small coordinate balls are normal neighborhoods of each of their points
The joint exponential map: smoothness, invertible differential at the diagonal, and the small-velocity two-point inverse
Normal neighborhoods, convex normal sets, the position vector and the squared-displacement function
The Lorentzian Gauss lemma and the radial maximum of proper time
The standard flat function
The standard flat function is smooth and flat at zero
The chain rule for total derivatives:
and smooth maps between smooth manifolds
The differential of a smooth map
The inverse metric, musical isomorphisms and index raising
Timelike, null, spacelike and causal vectors of a Lorentz vector space
The timelike set has exactly two convex components, described in orthonormal coordinates
Observers, rest spaces and the spatial projection at an event
The geodesic initial-value problem and the exponential map of the metric-selected connection
Covariant differentiation along curves: metric pairing, parallel transport and geodesic speed
Chart independence, concatenation, reparametrization and transitivity for causal curves
The push-up rule: p << q and q <= r imply p << r, together with the timelike-piece criterion
A Euclidean bump for a compact set inside an open set
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
Smooth partitions of unity subordinate to an open cover
Continuity of at a point of and on : the - condition, its agreement with at a limit point, and continuity at an isolated point
Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
The Axiom of Countable Choice ()
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
Local comparison of a riemannian metric with the euclidean metric
Riemannian distance on a connected manifold