Kaydedildi:
| Yazar: | |
|---|---|
| Materyal Türü: | Recurso digital |
| Dil: | En |
| Baskı/Yayın Bilgisi: |
Zenodo
2026
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| Konular: | |
| Online Erişim: | https://doi.org/10.5281/zenodo.20304729 |
| Etiketler: |
Etiketle
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İçindekiler:
- <p>[This is a pre-preprint for discussion only. I have no intention of submitting to a journal. If you have useful contributions or corrections please contact me, I would like to find a co-author, then I would consider submitting for peer review..]</p> <p>We introduce a topological 4-geon interpretation of the conformal big bang in which the ultraviolet limit is not a regime in which quantum mechanics needs discrete space models, but rather is a regime in which the ordinary stochastic cobordism boundary theory loses its stable, or persistent, complex structure. The physical ontology is taken to be a four-dimensional cobordism with microscopic wormhole topology in the interior. Quantum mechanics is then an effective boundary transform theory of wormhole-channel open cobordisms: spinors and Fradkin--Tseytlin scalar endomorphisms act on boundary data, while the bulk cobordism supplies the real geometric channel structure. In this setting, the complex phase of the boundary Clifford transform is directly seen as the algebraic inducement of the stochastic effects of a regulated wormhole sector. We formulate the conjecture that, as the conformal big bang is approached, microscopic wormhole-entanglement channels do not disappear, but their persistence time tends to the local effective Planck time in any scale-fixed frame, or equivalently that the dimensionless persistence number for phase-bearing channels tends to order unity. The boundary transform description is therefore repeatedly reset: persistent interference channels constantly break down and reform. <br>We outline a gauge-gravity formulation using the position gauge field $h$ and rotational gauge field $\omega$, and identify the Fradkin--Tsyetlin sector with dimension-zero scalar endomorphisms of the spinor--frame coupling, eliminating the need for an ordinary propagating Higgs field for conformal symmetry breaking.</p>