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Demonstrates how fermions as standing waves on a Möbius loop lead to a fundamental fermionic state, suggesting a topological link between fermions and bosons.
We propose that fermions are standing waves on a closed loop with Möbius topology. The non-orientable structure of the Möbius strip (classified by the first Stiefel-Whitney class w₁ = 1) imposes an anti-periodic boundary condition: f(θ + 2π) = −f(θ) This topological constraint permits only odd mode numbers n = 1, 3, 5, ..., providing a direct geometric origin for fermionic statistics. The Fundamental n = 3 Mode Invoking the Principle of Minimal Complexity, nature selects the lowest-energy non-trivial standing wave. While n = 1 is the lowest odd mode, it is rejected as "trivial" because it lacks internal spatial nodes. The preferred mode is: n = 3: Featuring three nodes and three antinodes distributed symmetrically around the loop. We argue that n = 3 is the fundamental fermionic state, serving as the geometric foundation for: Half-integer spin (L = 3/2 ħ). The sign change under a 2π rotation (the spinor property). The Pauli exclusion principle, which emerges from the anti-periodicity of the wave function. Fermion-Boson Bridge A key result of this paper is the Cutting Theorem: When a Möbius loop carrying the n = 3 fermionic mode is cut along its centreline, it unfolds into a double-twist strip (orientable, w₁ = 0) of twice the circumference. This operation transforms the standing wave into an n = 6 bosonic configuration, providing a topological link between the two sectors of particle physics. This work, alongside its companion paper on the Riemann–Silberstein vector, suggests a unified framework where the distinction between fermions and bosons reduces to the orientability of the underlying topology.
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Zheng Yan (2026) studied this question.
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