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The Geroch volume function: a continuous strictly increasing time function whose levels are Cauchy sets

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 curve calculus and auxiliary-length suppliers. Let (M,g,N) be a globally hyperbolic time-oriented smooth Lorentzian four-manifold (Chronology, causality, strong causality, global hyperbolicity and time functions clause (c)) and let μ be the volume measure of Existence of a positive smooth volume density of total mass one on a smooth Lorentzian four-manifold with μ(M)=1, μ(O)>0 for every nonempty open O and μ(E)=0 for every chart-Lebesgue-null Borel set. Let L:=ln⁡ denote the natural logarithm (The natural logarithm as the inverse of the exponential function) and define the volume time function t:M⟶R,t(p):=L(μ(I−(p)))−L(μ(I+(p)))=ln⁡μ(I−(p))μ(I+(p)). Then:

(a) t is well defined and continuous on M;

(b) t is strictly increasing along causal relations: if p≤q with p≠q, then t(p)<t(q); in particular t is a time function in the sense of Chronology, causality, strong causality, global hyperbolicity and time functions clause (d);

(c) for every inextendible future-directed causal curve γ:I→M one has lim⁡s→sup⁡It(γ(s))=+∞,lim⁡s→inf⁡It(γ(s))=−∞;

(d) every level set t−1(c), c∈R, is a Cauchy set (Spacelike hypersurfaces, acausal sets, Cauchy sets, domains of dependence and Cauchy horizons clause (c)); in particular it is acausal, and it is met in exactly one parameter value by every inextendible causal curve.

No smoothness of t is asserted.

Facts & Assumptions

Given: Countable Choice, Dependent Choice, a globally hyperbolic (M,g,N), the volume measure μ, the function t, and an inextendible future-directed causal curve γ:I→M.

[L1]

There is no nonconstant closed future causal curve, and no closed causal curve at all: strong causality fails at a point lying on such a curve, because the curve has a point other than the base point and therefore leaves and re-enters every sufficiently small neighbourhood of the base point (Chronology, causality, strong causality, global hyperbolicity and time functions clauses (b) and (c)).

[L2]

The volume functions are continuous and strictly monotone in the following form: for pk→p one has μ(I±(pk))→μ(I±(p)); the sets I±(x) are open with 0<μ(I±(x))<1; for p≪q one has μ(I−(p))<μ(I−(q)) and μ(I+(p))>μ(I+(q)); if x≪p then x≪q for every q≥p and dually (Continuity and strict monotonicity of the chronological volume functions in a globally hyperbolic manifold clauses (a)-(d), The push-up rule: p << q and q <= r imply p << r, together with the timelike-piece criterion clauses (a) and (b)).

[L3]

The causal relation ≤ is closed: pk≤qk, pk→p, qk→q implies p≤q; the sets J±(x) are closed (In a globally hyperbolic manifold the causal relation is closed and truncated causal cones over compact sets are compact clause (a)).

[L4]

Through every point x there are past and future timelike geodesic segments: for every sufficiently small ε>0 the points xε−:=exp⁡x(−εNx) and xε+:=exp⁡x(εNx) are defined with xε−≪x≪xε+; a causal curve is not constant on a nondegenerate parameter interval (Observers, rest spaces and the spatial projection at an event, The geodesic initial-value problem and the exponential map of the metric-selected connection clauses (a) and (d), Covariant differentiation along curves: metric pairing, parallel transport and geodesic speed clause 3, Causal curves, chronological and causal reachability, and inextendibility clause (b)).

[L5]

In this proof fix h to be the complete conformal metric h′ 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 clauses (b)-(d), and use that same metric for every length and distance. Strong causality bounds auxiliary lengths: for every compact K there is L(K)<∞ such that every future causal curve with image in K has h-length at most L(K); the auxiliary metric h is complete on each connected component and its distance induces the topology (Strong causality bounds the auxiliary length of causal curves contained in a compact set, 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).

[L6]

For a compact subarc, the Riemannian distance between its endpoints is at most its h-length, by the absolutely continuous distance-length inequality proved in 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 step 1.2 (Riemannian distance on a connected manifold, Riemannian distance is a metric). A Cauchy sequence in a connected component converges under the complete auxiliary metric (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 clause (c)). No arbitrary increasing reparametrization is asserted to preserve absolute continuity.

[L7]

Measure continuity from above: for a decreasing sequence of measurable sets An with μ(An0)<∞ one has μ(⋂nAn)=inf⁡nμ(An) (Continuity from above when one set has finite measure). The logarithm L=log⁡ is continuous, strictly increasing and onto R, with L(1)=0 (The natural logarithm as the inverse of the exponential function, Order, continuity, range, and the product, quotient, and reciprocal laws for the natural logarithm); consequently L(x)→−∞ as x→0+ and L(x)→+∞ as x→+∞, because for every real M the level xM>0 with L(xM)=M exists by surjectivity and strict increase gives L(x)<M for all 0<x<xM and L(x)>M for all x>xM. Intermediate values of a continuous real function on a connected domain are attained (A real-valued continuous map on a connected space has order-convex image, so it takes every value between any two of its values).

Proof

technique · direct
1.1L1L2L3L4

(Well-definedness.) Let p∈M. The set I−(p) is open and nonempty (it contains the points xε−≪p of [L4]), so 0<μ(I−(p)) by positivity of the measure [L2]; and μ(I−(p))<1: the point xε+≫p of [L4] does not lie in J−(p), because xε+≤p together with p≪xε+ would produce a nonconstant closed causal curve through p, contradicting [L1]; since J−(p) is closed by [L3] and xε+∉J−(p), a whole neighbourhood of xε+ is disjoint from I−(p), so μ(I−(p))≤1−μ(that neighbourhood)<1. The same holds for I+(p). Hence 0<μ(I±(p))<1 and t(p) is a well-defined real number.

1.2L5L6L7given

(Future decay of the future volumes.) Let γ:I→M be future-inextendible and fix s0∈I. The family {I+(γ(s))}s≥s0 is decreasing, and each term has measure at most one. Suppose inf⁡s≥s0μ(I+(γ(s)))≥ε>0 for some ε. Choose an increasing cofinal sequence sj in the future parameter tail (a real interval admits one). The decreasing sequence I+(γ(sj)) has intersection A:=⋂s≥s0I+(γ(s)) by cofinality and nesting. Measure continuity from above [L7] gives μ(A)≥ε, so A≠∅; choose z∈A, so that γ(s)≪z for all s≥s0. Then γ([s0,sup⁡I))⊆J+(γ(s0))∩J−(z), a compact causal diamond, so by [L5] the h-length of every subcurve of γ is at most L(K)<∞ with K:=J+(γ(s0))∩J−(z). Put F(s)=ℓh(γ∣[s0,s]) and L∞=sup⁡s≥s0F(s)≤L(K). Integral additivity gives ℓh(γ∣[s,t])=F(t)−F(s)≤L∞−F(s) for s<t, which tends to zero as s→sup⁡I. Hence [L6] makes the image points along an increasing cofinal parameter sequence Cauchy; they converge to z0 by completeness. The same distance bound and cofinality show that the entire tail γ(s) tends to z0, contradicting future-inextendibility. No change of parametrization is needed. Therefore μ(I+(γ(s)))→0 as s→sup⁡I.

2.1step 1.1L2L7

(Continuity.) If pk→p then μ(I±(pk))→μ(I±(p)) by [L2], and the logarithm is continuous on (0,∞) by [L7]; the difference of two continuous functions is continuous, so t is continuous. This proves (a).

2.2step 1.1L1L2L3L4L7

(Strict monotonicity.) Let p≤q with p≠q and choose a future causal curve γ:[0,1]→M with γ(0)=p, γ(1)=q. Fix s0∈(0,1) and put x:=γ(s0); then p≤x≤q, and p≠x, x≠q because equality would give a nonconstant closed causal subcurve, contrary to [L1]. We show μ(I−(q))>μ(I−(p)) and μ(I+(p))>μ(I+(q)). For the first: I−(p)⊆I−(q), since y≪p≤q gives y≪q by [L2]. If I−(q) were contained in J−(p), then for every point xε−≪x of [L4] we would have xε−≪x≤q, hence xε−≪q and therefore xε−∈I−(q)⊆J−(p), that is, xε−≤p; letting ε↓0 and using closedness of ≤ [L3] gives x≤p, which with p≤x yields a nonconstant closed causal curve through x (nonconstant because p≠x), contradicting [L1]. Hence I−(q)∖J−(p) is nonempty; it is open (as the intersection of the open I−(q) with the complement of the closed J−(p)) and is contained in I−(q)∖I−(p), so it has positive μ-measure, and additivity gives μ(I−(q))≥μ(I−(p))+μ(I−(q)∖J−(p))>μ(I−(p)). For the second: I+(q)⊆I+(p) by the dual push-up, and if I+(p)⊆J+(q) then every xε+≫x satisfies xε+≫x≥p, hence xε+≫p and xε+∈I+(p)⊆J+(q), that is xε+≥q; closedness of ≤ gives x≥q, which with x≤q is again a closed causal curve, contradicting [L1]. So I+(p)∖J+(q) is a nonempty open subset of I+(p)∖I+(q) and μ(I+(p))>μ(I+(q)). Since L is strictly increasing, t(p)=L(μ(I−(p)))−L(μ(I+(p)))<L(μ(I−(q)))−L(μ(I+(q)))=t(q). This proves (b).

2.3step 1.1step 1.2L2L7given

(Future growth of the past volumes and the limit at the future end.) With γ, s0 as in step 1.2: for s≥s0 one has I−(γ(s0))⊆I−(γ(s)) because y≪γ(s0)≤γ(s) gives y≪γ(s) by [L2], hence μ(I−(γ(s)))≥c:=μ(I−(γ(s0)))>0 by monotonicity and step 1.1. Combining with step 1.2, t(γ(s))=L(μ(I−(γ(s))))−L(μ(I+(γ(s))))≥L(c)−L(μ(I+(γ(s)))). Since μ(I+(γ(s)))→0+ and the logarithm tends to −∞ at 0+ [L7], the second term satisfies −L(μ(I+(γ(s))))→+∞, while L(μ(I−(γ(s))))≥L(c) remains bounded below; hence t(γ(s))→+∞ as s→sup⁡I.

3.1step 1.2step 2.3given

(The limit at the past end.) Apply steps 1.2 and 2.3 in the time-reversed orientation: the time reverse of γ is future-inextendible, its future volumes are the I−-volumes of γ, and its past volumes the I+-volumes; hence μ(I−(γ(s)))→0 as s→inf⁡I and, with μ(I+(γ(s)))≥μ(I+(γ(s1)))>0 for s≤s1, one gets t(γ(s))→−∞ as s→inf⁡I. This proves (c) for future-directed curves; a past-directed inextendible causal curve becomes future-directed after reversing its parameter, and the limits are interchanged accordingly.

4.1step 2.2step 2.3step 3.1L1L7∎

(Level sets are Cauchy.) Let c∈R and let γ:I→M be inextendible and causal; reversing the parameter if necessary, assume it is future-directed. By step 2.3 and step 3.1 the continuous function s↦t(γ(s)) on the interval I tends to +∞ at sup⁡I and to −∞ at inf⁡I; since the intermediate value theorem [L7] applies to continuous real functions on connected domains, for every c between the two limits there is s∈I with t(γ(s))=c. Hence every level set is met at least once. It is met at most once: if s1<s2 with t(γ(s1))=t(γ(s2))=c, then γ(s1)≤γ(s2) with γ(s1)≠γ(s2) (equality would be a nonconstant closed causal curve on [s1,s2], contradicting [L1]), so strict monotonicity, step 2.2, gives t(γ(s1))<t(γ(s2)), a contradiction. Therefore every inextendible causal curve meets t−1(c) in exactly one parameter value, so t−1(c) is a Cauchy set; acausality is the special case of two points y≤y′ of the level set with y≠y′, which strict monotonicity forbids. This proves (d).

Remarks

Depends on

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