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Time functions as utilities

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abstract

Every time function on spacetime gives a (continuous) total preordering of the spacetime events which respects the notion of causal precedence. The problem of the existence of a (semi-)time function on spacetime and the problem of recovering the causal structure starting from the set of time functions are studied. It is pointed out that these problems have an analog in the field of microeconomics known as utility theory. In a chronological spacetime the semi-time functions correspond to the utilities for the chronological relation, while in a K-causal (stably causal) spacetime the time functions correspond to the utilities for the K^+ relation (Seifert's relation). By exploiting this analogy, we are able to import some mathematical results, most notably Peleg's and Levin's theorems, to the spacetime framework. As a consequence, we prove that a K-causal (i.e. stably causal) spacetime admits a time function and that the time or temporal functions can be used to recover the K^+ (or Seifert) relation which indeed turns out to be the intersection of the time or temporal orderings. This result tells us in which circumstances it is possible to recover the chronological or causal relation starting from the set of time or temporal functions allowed by the spacetime. Moreover, it is proved that a chronological spacetime in which the closure of the causal relation is transitive (for instance a reflective spacetime) admits a semi-time function. Along the way a new proof avoiding smoothing techniques is given that the existence of a time function implies stable causality, and a new short proof of the equivalence between K-causality and stable causality is given which takes advantage of Levin's theorem and smoothing techniques.

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2026 1

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representative citing papers

Global hyperbolicity meets order completeness

gr-qc · 2026-08-04 · conditional · novelty 8.0

In smooth/C^{1,1} Lorentzian spacetimes, future/past chrono- and causalcompleteness and bounded directed order completeness are all equivalent to global hyperbolicity.

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  • Global hyperbolicity meets order completeness gr-qc · 2026-08-04 · conditional · none · ref 22 · internal anchor

    In smooth/C^{1,1} Lorentzian spacetimes, future/past chrono- and causalcompleteness and bounded directed order completeness are all equivalent to global hyperbolicity.