Proposes a principle explaining quantization in fermionic matter, highlighting π's role in quantum states.
The standard formulation of quantum mechanics relies on the Schrödinger equation and the Born rule but lacks a unified principle explaining why discreteness appears so universally. This paper proposes the Phase Quantization Principle: in any finite system, the total phase accumulated over a closed process must be a rational multiple of π. This is the necessary and sufficient condition for quantization. The special status of π does not arise from convention but from two structural facts: the topology of the three-dimensional rotation group SO(3) — whose fundamental group is Z₂ — and the spin-statistics of fermions, which acquire a phase of π under 2π rotation. π is therefore the minimum non-trivial physical phase in three spatial dimensions. The paper's primary new contribution is a phase-stability account of decoherent state selection: not only why superpositions disappear, but why the surviving definite states are those specific values. Four classes of quantum phenomena — energy quantization, geometric (Berry) phase, particle statistics, and post-decoherence state selection — are shown to be expressions of the same phase-closure condition.
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Chen et al. (2026) studied this question.
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