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Wormhole Nucleation from Anti-de Sitter vs Hartle-Hawking No-Boundary

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Quantum Tunneling Origin · within family
Wormhole Nucleation from Anti-de Sitter
2024 / 2026 · Speculative
Hartle-Hawking No-Boundary
1983 · Speculative
Proposed
2024 / 2026
1983
Key figures
Panos Betzios, Olga Papadoulaki, George Lavrelashvili, Jean-Luc Lehners
James Hartle, Stephen Hawking
In one sentence
A wave function for the universe in which a Euclidean wormhole, anchored in an anti-de Sitter region, gives birth to an expanding universe that begins with inflation.
The universe has no temporal boundary at the beginning. In Euclidean time, the universe is a smooth four-dimensional surface with no edge, like asking what is south of the South Pole.
Predictions
  • A small shift and faint oscillations in the [[cosmic microwave background]] on the largest angular scales, with a size set by the wormhole's charge
  • Short-wavelength fluctuations identical to those of standard inflation, so the signature appears only on the largest scales
  • Wormholes with small charge give a longer phase of inflation than wormholes with large charge
  • No initial [[singularity]]
  • Universe wavefunction smooth at a = 0
  • Predicts a specific spectrum of cosmological perturbations
Where it breaks
  • Lavrelashvili and Lehners find that no-boundary instantons still dominate the overall probability, which weakens the case that wormholes are the preferred beginning.
  • The universe needs a parent anti-de Sitter or flat region to emerge from, which moves the question of origins back one step.
  • The predicted signal sits on the largest scales of the sky, where there are too few independent patches to measure it precisely.
  • Feldbrugge, Lehners, Turok (2017) argue the proposal predicts an unstable universe
  • Direction of "outgoing" vs "incoming" mode is contested
  • A more careful mathematical analysis of the path integral suggests deeper problems, hinting the proposal may predict unstable outcomes (see Go Deeper)
  • Maldacena (2024) re-examines the no-boundary proposal and finds it predicts spatial curvature in conflict with observations, and is non-normalizable for landscape-like potentials.
  • Ivo, Li & Maldacena (2024) show that once you account for the regions of space we cannot observe, the mathematics of the no-boundary state leads to physically unrealistic predictions, sharpening the case against the original proposal.
Key unresolved problem
Which beginning wins: the wormhole, or the no-boundary instanton it turns into at zero charge. Current calculations still favour no-boundary overall, so the wormhole route needs a reason to be selected.
The instability problem: a careful redo of the math by Feldbrugge, Lehners, and Turok suggests the no-boundary proposal predicts runaway, ever-growing fluctuations, which would mean an unstable universe rather than the smooth one we see.
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