Relational bundle geometric formulation of non-relativistic quantum mechanics
J. François, L. Ravera
TL;DR
This work presents a geometric, bundle-based reformulation of non-relativistic quantum mechanics using cocyclic bundle geometry, where wavefunctions are cocyclic 0-forms on configuration-space-time and Schrödinger dynamics arise from a flat cocyclic covariant derivative tied to a cocyclic connection. The Dirac–Feynman path integral naturally emerges from this framework, linking classical action to a cocyclic structure and enabling a Lagrangian view of QM. The Dressing Field Method is employed to derive a relational formulation, yielding basic cocyclic fields that encode relational degrees of freedom and provide covariance under changes of physical reference frames. The approach yields a relational quantum mechanics with a clear notion of frame covariance and a relational path integral, offering a quantum-democratic viewpoint in which any subsystem can serve as a reference without privileging an external observer. Potential extensions include relatiionalizing spins, extended bodies, and a relativistic version, with a broader program of relational quantization across physics.
Abstract
We present a bundle geometric formulation of non-relativistic many-particles Quantum Mechanics. A wave function is seen to be a $\mathbb{C}$-valued cocyclic tensorial 0-form on configuration space-time seen as a principal bundle, while the Schrödinger equation flows from its covariant derivative, with the action functional supplying a (flat) cocyclic connection 1-form on the configuration bundle. In line with the historical motivations of Dirac and Feynman, ours is thus a Lagrangian geometric formulation of QM, in which the Dirac-Feynman path integral arises in a geometrically natural way. Applying the dressing field method, we obtain a relational reformulation of this geometric non-relativistic QM: a relational wave function is realised as a basic cocyclic 0-form on the configuration bundle. In this relational QM, any particle position can be used as a dressing field, i.e. as a "physical reference frame". The dressing field method naturally accounts for the freedom in choosing the dressing field, which is readily understood as a covariance of the relational formulation under changes of physical reference frame.
