Why the Framework Is Affine: Cross-Sector Coupling, the Kaluza-Klein Tower, and the Origin of Apparent Sector Independence

The G2 framework is multi-sector: its forces and properties are separate broken sectors rather than subgroups of a single group, a structure forced by the rank of G2, which cannot accommodate the full Standard Model gauge group. This raises a question the framework has not previously answered: if the sectors are genuinely separate, how do they couple, as they must, since quarks and leptons interact and the Standard Model is a single connected theory? We argue that the answer explains a feature of the framework otherwise taken as given — that it is not merely G2 but the affine extension of SO(8). The rank obstruction that separates the sectors in the finite algebra is lifted in the affine extension, which is infinite-dimensional and can contain the couplings the finite algebra cannot. Cross-sector coupling therefore lives in the affine layer and the affine extension is necessary rather than decorative: it is what makes a multi-sector theory consistent. We identify the affine mode tower with the Kaluza-Klein tower of the framework’s compactification, placing the mediating states at the compactification scale of order ten to the sixteenth GeV. This has an immediate consequence: cross-sector effects are suppressed at low energy by the square of the ratio of the energy to the Kaluza-Klein scale, which is why the sectors appear independent to us. Proton decay, a cross-sector process, is the low-energy window onto this coupling and its predicted rate uses the same scale, a self-consistency we note. The same scale organises the observable cross-sector physics by the number of sector-crossings a process requires: the neutrino mass, a single-crossing effect, comes out at the observed scale, proton decay is the two-crossing effect and every other cross-sector process requires more crossings and is suppressed beyond observability — a sparse phenomenology of two windows and no others, falsifiable by any further cross-sector signal. We present the architecture as a structural proposal and are explicit that the identification of the affine tower with the compactification tower is well motivated within the framework but requires the compactification details to establish rigorously.

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-10-27
DOI
https://doi.org/10.5281/zenodo.23691951
Primary Topic
Particle physics theoretical and experimental studies
Type
preprint
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preprint

Why the Framework Is Affine: Cross-Sector Coupling, the Kaluza-Klein Tower, and the Origin of Apparent Sector Independence

Vali Ilyas
5 links
Zenodo (CERN European Organization for Nuclear Research)
Particle physics theoretical and experimental studies
preprint

Why the Framework Is Affine: Cross-Sector Coupling, the Kaluza-Klein Tower, and the Origin of Apparent Sector Independence

Vali Ilyas
preprint en

Abstract

The G2 framework is multi-sector: its forces and properties are separate broken sectors rather than subgroups of a single group, a structure forced by the rank of G2, which cannot accommodate the full Standard Model gauge group. This raises a question the framework has not previously answered: if the sectors are genuinely separate, how do they couple, as they must, since quarks and leptons interact and the Standard Model is a single connected theory? We argue that the answer explains a feature of the framework otherwise taken as given — that it is not merely G2 but the affine extension of SO(8). The rank obstruction that separates the sectors in the finite algebra is lifted in the affine extension, which is infinite-dimensional and can contain the couplings the finite algebra cannot. Cross-sector coupling therefore lives in the affine layer and the affine extension is necessary rather than decorative: it is what makes a multi-sector theory consistent. We identify the affine mode tower with the Kaluza-Klein tower of the framework’s compactification, placing the mediating states at the compactification scale of order ten to the sixteenth GeV. This has an immediate consequence: cross-sector effects are suppressed at low energy by the square of the ratio of the energy to the Kaluza-Klein scale, which is why the sectors appear independent to us. Proton decay, a cross-sector process, is the low-energy window onto this coupling and its predicted rate uses the same scale, a self-consistency we note. The same scale organises the observable cross-sector physics by the number of sector-crossings a process requires: the neutrino mass, a single-crossing effect, comes out at the observed scale, proton decay is the two-crossing effect and every other cross-sector process requires more crossings and is suppressed beyond observability — a sparse phenomenology of two windows and no others, falsifiable by any further cross-sector signal. We present the architecture as a structural proposal and are explicit that the identification of the affine tower with the compactification tower is well motivated within the framework but requires the compactification details to establish rigorously.

Zenodo (CERN European Organization for Nuclear Research)
Particle physics theoretical and experimental studies
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Why the Framework Is Affine: Cross-Sector Coupling, the Kaluza-Klein Tower, and the Origin of Apparent Sector Independence — Vali Ilyas · Zenodo (CERN European Organization for Nuclear Research) (2026) | TGRS Research Map | TGRS