Off-Shell Quantum Mechanics as Factorization Algebras on Intervals

TL;DR

This paper develops an off-shell formulation of quantum mechanics using factorization and BV algebras, demonstrating its equivalence to on-shell quantum mechanics for harmonic oscillators and spin-1/2 systems.

Contribution

It introduces a novel off-shell approach to quantum mechanics based on factorization algebras, extending previous work to include various interval types and spin systems.

Findings

Off-shell formulation is quasi-isomorphic to on-shell quantum mechanics.

Extended the framework to include half-open and closed intervals.

Generalized the approach to spin-1/2 systems.

Abstract

We present, for the harmonic oscillator and the spin-$\frac{1}{2}$ system, an alternative formulation of quantum mechanics that is `off-shell': it is based on classical off-shell configurations and thus similar to the path integral. The core elements are Batalin-Vilkovisky (BV) algebras and factorization algebras, following a program by Costello and Gwilliam. The BV algebras are the spaces of quantum observables ${\rm Obs}^q(I)$ given by the symmetric algebra of polynomials in compactly supported functions on some interval $I\subset\mathbb{R}$, which can be viewed as functionals on the dynamical variables. Generalizing associative algebras, factorization algebras include in their data a topological space, which here is $\mathbb{R}$, and an assignment of a vector space to each open set, which here is the assignment of ${\rm Obs}^q(I)$ to each open interval $I$. The central structure maps are bilinear ${\rm Obs}^q(I_1)\otimes {\rm Obs}^q(I_2)\rightarrow {\rm Obs}^q(J)$ for disjoint intervals $I_1$ and $I_2$ contained in an interval $J$, which here is the wedge product of the symmetric algebra. We prove, as the central result of this paper, that this factorization algebra is quasi-isomorphic to the factorization algebra of `on-shell' quantum mechanics. In this we extend previous work by including half-open and closed intervals, and by generalizing to the spin-$\frac{1}{2}$ system.