Loading article...
Loading article...
Stream/Area:
-
Subject:
-
Paper ID:
IJSREM66508
Volume:
10 |
8 |
Aug 2026
Pages:
1-21
Publication Frequency:
Monthly (12 issues per year)
License:International Journal of Scientific Research in Engineering and Management follows the Creative Commons Attribution 4.0 (CC BY 4.0) License, allowing free use and distribution with proper attribution.

Independent Researcher
Independent Researcher
We develop a single geometric premise—the imaginary unit read as a rotation generator (a rotor), with a source and a sink as its two fixed points—into an explicit construction of the discrete structure of the Standard Model (SM). A particle is modeled as a self-sustaining source–sink circulation; its charge is the pump direction, its spin the double-cover class of the rotor group, its hypercharge a net source/sink flux count, and its mass the winding density of a topological soliton. Combined with the division-algebra tower ℂ ⊗ ℍ (weak) and ℂ ⊗ 𝕆 (color and charge) and its exceptional Jordan closure 𝔍3(𝕆) (the 27-dimensional Albert algebra with automorphism group 𝐹4), this reproduces, computationally and without free parameters: color 𝑆𝑈(3); the electric-charge spectrum {0, 1⁄3 , 2⁄3 , 1}; the weak doublet with 𝐼3 = ± 1⁄2; the number of colors 𝑁𝑐 = 3; a single generation (not three) via 𝑆𝑝𝑖𝑛(8) triality; spin-1⁄2 and Fermi statistics from the quaternion group 𝑄8; the full hypercharge spectrum of one generation as a rigid integer flux-count pattern with zero free parameters, sealed by the vanishing of both anomaly traces at 𝑁𝑐 = 3; and the nucleon as a soliton whose stabilizing term is derived as the area strain-invariant of the rotor map, reproducing the Adkins–Nappi–Witten couplings. On the discrete-symmetry side we prove a positive and a negative result: a CP-odd invariant exists and is the three-rotor geometric (Bargmann) phase, equal to the solid angle of the rotors’ spherical triangle—the same object as the CKM unitarity-triangle area; whereas parity violation cannot arise from the construction, a 𝐶𝑃-lock we establish four independent ways. The Weyl chiral split itself is derived from the fluid boost (the transformation law of the current’s spinor square-root, 𝜓𝑅′ = 𝐵𝜓𝑅, 𝜓𝐿′ = 𝐵−1𝜓𝐿), and complexifying 𝔍3(𝕆) → 𝔍3(𝕆) ⊗ ℂ (structure group 𝐸6) makes a chiral generation representable rather than impossible. The QCD scale, the Yukawa sector, and the orientation of parity (a single input, unified by 𝐶𝑃𝑇) remain input—exactly as they do in the Standard Model. Every claim carries an executable verification and a ledger tag: FORCED, INPUT, or NEGATIVE.
KEYWORDS
From a single premise—a source, a sink, and the rotor between them—together with the division-algebra tower and its exceptional Jordan closure, a substantial and parameter-free block of the Standard Model’s discrete structure follows: the gauge group and color count, the electric-charge spectrum, the full hypercharge pattern of a generation as a rigid flux-count, spin-1⁄2, one generation, the nucleon as a soliton with a derived stabilizer, and the structural origin of CP violation as a geometric triangle area. Two integers organize the whole picture: 𝑁𝑐 = 3, which appears as the color count, the charge sum, both anomaly traces, and the fermion-statistics sign; and the quaternionic 𝑆𝑈(2), which supplies every 𝜋3 winding, including those inside the octonionic groups. What the geometry does not reach—the QCD scale, the Yukawa sector, the orientation of parity—it fails to reach for reasons we state precisely, and in each case the Standard Model fails identically. The claim is not that geometry is the complete origin of the Standard Model, but that it is the demonstrable origin of its discrete skeleton, with a boundary that is itself a theorem.
E. Wigner, “On an algebraic generalization of the quantum mechanical formalism,” Ann. of Math. 35, 29 (1934). A. A. Albert, “On a certain algebra of quantum mechanics,” Ann. of Math. 35, 65 (1934). M. Dubois-Violette, “Exceptional quantum geometry and particle physics,” Nucl. Phys. B 912, 426 (2016). I. Todorov, M. Dubois-Violette, “Deducing the symmetry of the standard model from the automorphism and structure groups of the exceptional Jordan algebra,” Int. J. Mod. Phys. A 33, 1850118 (2018). I. Todorov, “Octonions, exceptional Jordan algebra and the role of the group 𝐹4 in particle physics,” Adv. Appl. Clifford Algebras 28, 82 (2018). L. Boyle, “The Standard Model, the exceptional Jordan algebra, and triality,” arXiv:2006.16265 (2020). T. H. R. Skyrme, “A non-linear field theory,” Proc. R. Soc. A 260, 127 (1961). G. S. Adkins, C. R. Nappi, E. Witten, “Static properties of nucleons in the Skyrme model,” Nucl. Phys. B 228, 552 (1983). E. Witten, “Global aspects of current algebra,” Nucl. Phys. B 223, 422 (1983); “Current algebra, baryons, and quark confinement,” ibid. 223, 433 (1983). N. S. Manton, “Geometry of Skyrmions,” Commun. Math. Phys. 111, 469 (1987). J. Goldstone, F. Wilczek, “Fractional quantum numbers on solitons,” Phys. Rev. Lett. 47, 986 (1981). H. Georgi, C. Jarlskog, “A new lepton–quark mass relation in a unified theory,” Phys. Lett. B 86, 297 (1979). Y. Koide, “A new view of quark and lepton mass hierarchy,” Phys. Rev. D 28, 252 (1983). F. Gürsey, P. Ramond, P. Sikivie, “A universal gauge theory model based on 𝐸6,” Phys. Lett. B 60, 177 (1976).
Publication Date
8/4/2026
Peer Review Type
Double-Blind Peer Review
Review Rounds: 2
Documents
Article Views
0
Total views since publication
PDF Downloads
10
Total downloads since publication
Geographic Reach
5
Digital Preservation: This article is permanently archived on Zenodo and complies with all data preservation standards across major indexing platforms.
Plagiarism Screening
This manuscript has been checked for plagiarism using TurnitinPlagiarismChecker software.
Conflict of Interest
The authors declare no conflict of interest related to this research work.
Funding Information
No funding information available for this research.
Related research in the same subject area
Loading similar articles...