Nonlinear Boundaries in Quantum Mechanics
Arthur Davidson

TL;DR
This paper explores how nonlinear boundary conditions in quantum mechanics can restore gauge invariance on a ring, resulting in a continuous eigenvalue spectrum while preserving superposition and Hermiticity.
Contribution
It demonstrates that nonlinear boundaries can reconcile gauge invariance with eigenvalue spectra, challenging the traditional linear boundary assumption in quantum systems.
Findings
Nonlinear boundaries restore gauge invariance.
Eigenfunctions can have a continuous spectrum.
Superposition principle remains valid despite nonlinearity.
Abstract
Based on empirical evidence, quantum systems appear to be strictly linear and gauge invariant. This work uses concise mathematics to show that quantum eigenvalue equations on a one dimensional ring can either be gauge invariant or have a linear boundary condition, but not both. Further analysis shows that non-linear boundaries for the ring restore gauge invariance but lead unexpectedly to eigenfunctions with a continuous eigenvalue spectrum, a discreet subset of which forms a Hilbert space with energy bands. This Hilbert space maintains the principle of superposition of eigenfunctions despite the nonlinearity. The momentum operator remains Hermitian. If physical reality requires gauge invariance, it would appear that quantum mechanics should incorporate these nonlinear boundary conditions.
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Taxonomy
TopicsQuantum Mechanics and Applications · Experimental and Theoretical Physics Studies · Mechanical and Optical Resonators
