Quantum Dance at the Mirror Wall: Angular Momentum in a Closed Universe ✛ ✎

Original: "Orbital angular momentum can take non-integer values in a closed universe"
· Daniel Burgarth, Paolo Facchi
arXiv:2506.03254v1 · 2025-06-03 · arXiv non-exclusive · independent analysis · 3 min
In a closed universe, orbital angular momentum can take not only integer values but any value, from half-integers to irrationals.

A century ago, quantum mechanics gave the world a neat picture: a particle rotating around a point can only have certain discrete amounts of angular momentum, integer multiples of Planck's constant. This rule seemed as solid as the law of gravity, and it followed from simple algebraic arguments. But a new study shows that once you close up space, the angular momentum spectrum breaks, and values that were once thought forbidden appear.

In a closed universe, a particle can have orbital angular momentum equal to the square root of two times Planck's constant. Such a value is impossible in infinite space.

Think of quantum angular momentum as a dance on a stage with mirrored walls. In an ordinary room, a dancer spins in smooth circles, and each turn is a multiple of a full rotation. But if the walls are mirrors, then at the very edge of the stage, reflections merge with the original, and the dance gives rise to new figures. That is exactly what happens to a particle on a flat torus, a two-dimensional universe where opposite edges are identified. The authors considered a quantum particle in such a space and decomposed its states into classical rotational orbits. It turns out that besides the familiar circular orbits, there are 'edge' orbits that, due to the periodic boundaries, look like broken arcs. These orbits generate the continuous band in the spectrum.

The orbital angular momentum spectrum in a closed universe consists of two parts. The first is the usual integer values, as in textbooks. The second is a continuous band from minus infinity to minus ħ and from ħ to plus infinity. In this band, there are values that were previously considered forbidden: half-integers and even irrationals. The effect does not depend on the size of the universe; it is caused by global topology, not local properties. The states of the continuous spectrum are localized away from the center of rotation, at the 'edge' of space, and have opposite chirality.

The size of the universe does not affect the spectrum: the effect is due to topology, not geometry.

This is the first example where the global structure of space gives rise to a continuous component in the spectrum of a fundamental observable. Previously, it was thought that orbital angular momentum is always quantized in integers, and that this follows from commutation relations alone. Now it is clear that algebraic proofs are incomplete; they do not account for the topology of space. Practical applications are not yet in sight, but the result connects quantum mechanics with cosmology and string theory, where compactified dimensions are common. If our universe has the shape of a torus, photons with non-integer orbital angular momentum could have left a trace in the polarization of the cosmic microwave background. Future observations might see this dance at the mirror wall.

In a closed universe, a particle can have orbital angular momentum equal to the square root of two times Planck's constant. Such a value is impossible in infinite space.

The idea echoes Greg Egan's novel 'Diaspora', where physics in closed universes with nontrivial topology leads to unusual quantum effects.

L_z = m\hbar, \quad m \in \mathbb{Z}
In infinite space, the orbital angular momentum along the z-axis is quantized: it takes only integer values m times Planck's constant ħ.
|L_z| \geq \hbar
In a closed universe, a continuous band of angular momentum values appears outside the interval from -ħ to ħ. In this band, the momentum can be anything, including half-integers and irrationals.
Scientists
Johannes KeplerIsaac NewtonEmmy NoetherWerner HeisenbergKip ThorneJohn Stewart Bell
Concepts
angular momentum orbital angular momentum quantum orbital motion spin axis commutator continuum probability organic molecules in space vacuum nuclear spin orbit Hilbert space rotation period wavenumber vacuum energy uncertainty principle ring quantum number spin