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Temporal functions are time functions, and time functions forbid closed causal curves
Statement
Assume the Axioms of 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). Let be a time-oriented smooth Lorentzian four-manifold, let be a temporal function on it in the sense of Chronology, causality, strong causality, global hyperbolicity and time functions clause (e), and write for its gradient. Then:
(a) for every nonzero future causal vector .
(b) For every future causal curve in the class of Causal curves, chronological and causal reachability, and inextendibility, the composite is locally absolutely continuous, its derivative satisfies at almost every , and consequently
(c) is a time function on in the sense of Chronology, causality, strong causality, global hyperbolicity and time functions clause (d); every level set , , is achronal; and is causal and chronological: it admits no nonconstant future causal curve with equal endpoints.
Facts & Assumptions
Given: The choice assumptions, a temporal function with gradient , a future causal curve , and real numbers in .
An observer is a future-directed unit timelike vector , and for every observer and every nonzero future causal vector at the same point one has (Pairing of an observer with future causal vectors, Observers, rest spaces and the spatial projection at an event).
The gradient exists and is unique with for every smooth vector field , because is nondegenerate; and for every (The inverse metric, musical isomorphisms and index raising, The differential of a smooth map, Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model).
The temporal condition is and (Chronology, causality, strong causality, global hyperbolicity and time functions clause (e)); a vector with and is past-directed timelike, and is then an observer (Timelike, null, spacelike and causal vectors of a Lorentz vector space, Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model).
For a future causal curve , the set of at which exists, is nonzero and is future causal has full measure in ; the composite of with a smooth function on is locally absolutely continuous and the chain rule holds at almost every (Chart independence, concatenation, reparametrization and transitivity for causal curves clauses (b) and (c), Causal curves, chronological and causal reachability, and inextendibility clause (b)).
For absolutely continuous, under the choice assumptions: is differentiable almost everywhere, , and (Fundamental theorem of calculus for absolutely continuous functions, Absolute continuity on a compact interval).
If almost everywhere and , then almost everywhere (A nonnegative measurable function has integral exactly when it vanishes almost everywhere).
Proof
(Pairing of the gradient with future causal vectors.) Put . By [L3], and , so is past-directed timelike and satisfies and ; that is, is an observer. Let be any nonzero future causal vector; by [L1], , that is , hence . By [L2] this is , which proves (a).
(The composite and its derivative.) Apply [L4] with the scalar target and smooth map . The composite is locally absolutely continuous and at almost every . At every such at which in addition is nonzero and future causal, (a) gives ; by [L4] the set of such has full measure, so almost everywhere, and in particular the derivative is everywhere nonnegative almost everywhere.
(Strict monotonicity.) Let and suppose that is not constant on ; restrict to , a future causal curve. Put , which is absolutely continuous by step 2.1. By [L5], . Suppose for contradiction that . By [L5] and step 2.1, with almost everywhere, so [L6] gives almost everywhere on . On the other hand, the set of at which is nonzero future causal has full measure in , and at each such point by (a), so on a nonempty full-measure set, contradicting almost everywhere. Hence , which is the inequality of (b).
(Time function, achronality and causality.) By step 3.1, is a time function in the sense of clause (d) of Chronology, causality, strong causality, global hyperbolicity and time functions. If , choose a future timelike curve from to ; it is not constant on its parameter interval, because on a nondegenerate interval it has nonzero future timelike velocity at almost every parameter value (Causal curves, chronological and causal reachability, and inextendibility clause (b)), so step 3.1 gives . Hence two distinct points of a level set are never chronologically related in either direction, that is, every level set is achronal. If is a nonconstant future causal curve with , then and step 3.1 gives , a contradiction; hence no such curve exists, and is causal and chronological by clause (a) of Chronology, causality, strong causality, global hyperbolicity and time functions. This proves (c) and completes the proof.
Remarks
- Hypotheses. The proof uses only the temporal condition, the choice assumptions carried by the absolutely continuous fundamental theorem of calculus, and the causal-curve calculus; no completeness, compactness or dynamical hypothesis enters.
- Sharpness. The lemma gives no converse: a causal spacetime need not admit a temporal function, and a time function need not be smooth or have timelike gradient; the construction of smooth temporal functions on globally hyperbolic spacetimes is a separate theorem.
Depends on
Chronology, causality, strong causality, global hyperbolicity and time functions
Causal curves, chronological and causal reachability, and inextendibility
Chart independence, concatenation, reparametrization and transitivity for causal curves
Smooth time-oriented Lorentzian four-manifolds: the geometric objects of the model
The inverse metric, musical isomorphisms and index raising
The differential of a smooth map
Pairing of an observer with future causal vectors
Observers, rest spaces and the spatial projection at an event
Fundamental theorem of calculus for absolutely continuous functions
A nonnegative measurable function has integral exactly when it vanishes almost everywhere
The Axiom of Countable Choice ()
The axiom of dependent choice: a relation in which every element is related to something admits an -indexed chain
Timelike, null, spacelike and causal vectors of a Lorentz vector space
Absolute continuity on a compact interval
Dependency tree · 2 levels
Sources
- E. Minguzzi, Lorentzian causality theory, Living Reviews in Relativity 22 (2019), article 3: isotone functions (Definition 1.17 printed p. 17), semi-time and time functions (Definitions 1.20-1.21 printed p. 18), temporal functions (Definition 1.22 and Theorem 1.23 printed p. 19), and stable causality, section 4.4 printed pp. 137-141
- S. M. Carroll, Lecture Notes on General Relativity, arXiv:gr-qc/9712019v1 (1997): the initial value formulation and domains of dependence, printed pp. 119-127 (PDF pp. 126-134)