Schrödinger's Hidden Variable: Resolving the 1944 "Collapse of Determinism" via the Discrete $A_4$ Lattice
The recent archival recovery and transcription of Erwin Schrödinger's unpublished 1944–1945 manuscript, Collapse of Determinism (Del Santo, 2026), revealed that Schrödinger formulated an explicit, deterministic hidden-variable threshold ($\lambda \ge \sin^2\theta$) and post-measurement state-update rule ($\lambda' = \frac{\lambda - \sin^2\theta}{\cos^2\theta}$) to refute E. T. Whittaker's claim that Malus's Law precludes determinism in quantum optics. While Schrödinger's continuous 1D algebraic model was mathematically exact for sequential single-photon polarizers, it lacked a physical microscopic substrate and remained vulnerable to later Bell-type locality arguments. In this manuscript, we demonstrate that Schrödinger's 1944 continuous equations are the exact macroscopic continuum shadows of the discrete hardware of the Dynamic Needle Framework (DNF). Modeling the photon as an untethered 1D topological string ($C_K = 0$) traversing the projected 5-dimensional $A_4$ quasicrystalline lattice over $\mathbb{Q}(\sqrt{5})$, we establish: Diophantine Quantization of $\lambda$: Rather than a continuous real variable requiring infinite information density, Schrödinger's hidden variable is strictly quantized over the finite 5D Hilbert flux capacity ($N_{flux} = 132^5 = 40,074,642,432$) of a macroscopic $k=1$ dodecahedral voxel: $\lambda_n = N_{aligned}/N_{flux} = 1 - \epsilon(t)$. Driven by the irrational Golden Ratio phase residue $\epsilon(t) = 2\vert{}\phi N(t) - \operatorname{round}(\phi N(t))\vert{}$, Weyl's Equidistribution Theorem guarantees that $\lambda_n$ is strictly uniformly distributed on $[0, 1]$ with a discrete step resolution of $\Delta\lambda = 132^{-5} \approx 2.495 \times 10^{-11}$, recovering Malus's Law from pure number theory without probabilistic postulates. Trace-Preserving Integer Renormalization: At a polarizing boundary via Discrete Exterior Calculus (DEC), a discrete orientation state $m$ partitions $N_{flux}$ into orthogonal blocked modes $N_\perp(m)$ and parallel transmitted modes $N_\parallel(m) = N_{flux} - N_\perp(m)$. When $N_{aligned} \ge N_\perp(m)$, the string pays the integer boundary toll $N_\perp(m)$ and renormalizes its remaining phase count against the restricted parallel pathway capacity to preserve unit trace under the Discrete Noether Theorem: $\lambda_n' = \frac{N_{aligned} - N_\perp(m)}{N_{flux} - N_\perp(m)} \longrightarrow \frac{\lambda_n - \sin^2\theta}{\cos^2\theta}$. Bypassing Bell's Theorem via the $k=4$ Protospace Colloid: Evaluating the DNF's recursive fractal spatial hierarchy ($S = 132^{20} \approx 2.579 \times 10^{42}$), we prove that at the 4th deflation step ($k=4$, $6.76 \times 10^{-142}\text{ m}$), the Lucas nodal demand ($L_{12} = \phi^{12} + \phi^{-12} = 322$) exceeds the $N = 137.030$ projection window limit, dissolving the spatial metric into the timeless, zero-metric protospace colloid where all entangled endpoints are universally adjacent ($d_{proto}(A,B) \equiv 0$). Routing Schrödinger's two-channel trace-preserving renormalization across a shared $C_K = 0$ protospace tether yields strictly unbiased local marginals ($P(A=\pm 1) = 1/2$, satisfying no-signaling) while transitioning the bipartite correlation from the classical local $L^1$ taxicab bound ($S_{L_1} = 2$) to the exact quadratic $L^2$ quantum correlation $E(\theta_A, \theta_B) = \cos(2(\theta_A - \theta_B))$, deterministically achieving Tsirelson's bound ($S_{CHSH} = 2\sqrt{2}$).
Authors
- William Hansen (ORCID: https://orcid.org/0009-0005-1707-5847)
Publication Details
- Journal
- Zenodo (CERN European Organization for Nuclear Research)
- Published
- 2026-11-06
- DOI
- https://doi.org/10.5281/zenodo.24021143
- Primary Topic
- Quantum Mechanics and Applications
- Type
- preprint