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Wormhole Nucleation from Anti-de Sitter vs The Boundary Proposal
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Wormhole Nucleation from Anti-de Sitter Speculative | The Boundary Proposal Speculative | |
|---|---|---|
| Proposed | 2024 / 2026 | 2024 |
| Key figures | Panos Betzios, Olga Papadoulaki, George Lavrelashvili, Jean-Luc Lehners | Bjoern Hassfeld, Arthur Hebecker |
| 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. | An alternative to Hartle-Hawking and Vilenkin in which the universe begins with a finite spacelike spherical boundary that can dominate over the no-boundary instanton. |
| Predictions |
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| Where it breaks |
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| 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 input-geometry problem: the proposal has to be handed the size of its starting boundary surface from outside, which critics say just moves the fine-tuning problem somewhere else rather than removing it. |
| Reader vote | No votes yet | No votes yet |
Wormhole Nucleation from Anti-de Sitter
2024 / 2026 · Speculative
The Boundary Proposal
2024 · Speculative
Proposed
2024 / 2026
2024
Key figures
Panos Betzios, Olga Papadoulaki, George Lavrelashvili, Jean-Luc Lehners
Bjoern Hassfeld, Arthur Hebecker
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.
An alternative to Hartle-Hawking and Vilenkin in which the universe begins with a finite spacelike spherical boundary that can dominate over the no-boundary instanton.
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
- Distinct primordial perturbation spectrum from Hartle-Hawking and Vilenkin proposals
- Specific signatures in the CMB tied to the boundary geometry
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.
- Requires specifying the boundary geometry as input, which some critics view as no improvement over the boundary conditions it replaces.
- The phenomenological implications are still being worked out and have not yet been compared to Planck data.
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 input-geometry problem: the proposal has to be handed the size of its starting boundary surface from outside, which critics say just moves the fine-tuning problem somewhere else rather than removing it.
Reader vote
No votes yet
No votes yet