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Inflationary spacetimes are not past-complete

8 Pith papers cite this work. Polarity classification is still indexing.

8 Pith papers citing it
abstract

Many inflating spacetimes are likely to violate the weak energy condition, a key assumption of singularity theorems. Here we offer a simple kinematical argument, requiring no energy condition, that a cosmological model which is inflating -- or just expanding sufficiently fast -- must be incomplete in null and timelike past directions. Specifically, we obtain a bound on the integral of the Hubble parameter over a past-directed timelike or null geodesic. Thus inflationary models require physics other than inflation to describe the past boundary of the inflating region of spacetime.

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citation-polarity summary

years

2026 5 2025 3

verdicts

UNVERDICTED 8

roles

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representative citing papers

Open case for a closed universe

hep-th · 2025-10-15 · unverdicted · novelty 6.0

A no-go theorem proves flat and open FRW universes cannot be nonsingular, geodesically complete and ANEC-consistent while closed universes can, with positive curvature mimicking phantom dark energy at the 1% level.

Geodesic completion of big bangs from emergent geometry

gr-qc · 2026-02-25 · unverdicted · novelty 5.0

Phantom Chaplygin gas forces the Einstein-frame lapse to change sign smoothly while the causal-frame lapse stays positive, yielding a robust non-singular bounce even with extra matter.

Geodesically Complete Curvature-Bounce Inflation

astro-ph.CO · 2026-04-29 · unverdicted · novelty 5.0

A closed k=+1 FRW universe with curvature-driven bounce and canonical scalar inflation remains sub-Planckian, satisfies the null energy condition, and produces ns=0.9617-0.9650 and r=0.0037-0.0045 consistent with data.

Inflation from a Weyl-flat null origin

hep-ph · 2026-04-19 · unverdicted · novelty 5.0

Single-field inflation with ε(N) approaching a constant in (0,1) at early times forms an asymptotic universality class with a Weyl-flat null origin while producing ns and r values compatible with Planck data.

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