Search arXivSearch

arXiv · 2412.06912

Off-Shell Quantum Mechanics as Factorization Algebras on Intervals

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.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Christoph Chiaffrino, Noah Hassan, Olaf Hohm. 2024-12-09. Off-Shell Quantum Mechanics as Factorization Algebras on Intervals. https://arxiv.org/abs/2412.06912

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Gaillard-Zumino non-invertible symmetries

We uncover an infinite class of novel zero-form non-invertible symmetries in a broad family of four-dimensional models, studied years ago by Gaillard and Zumino (GZ), which includes several extended supergravities as particular subcases. The GZ models consist of abelian gauge fields coupled to a neutral sector, typically including a set of scalars, whose equations of motion are classically invariant under a continuous group $\mathscr{G}$ acting on the electric and magnetic field strengths via symplectic transformations. The standard lore holds that, at the quantum level, these symmetries are broken to an integral subgroup $\mathscr{G}_\mathbb{Z}$. We show that, in fact, a much larger subgroup $\mathscr{G}_\mathbb{Q}$ survives, albeit through non-invertible topological defects. We explicitly construct these defects and compute some of their fusion rules. As illustrative examples, we consider the axion-dilaton-Maxwell model and the bosonic sector of a class of $\mathcal{N}=2$ supergravities of the kind that appear in type II Calabi-Yau compactifications. Finally, we comment on how (part of) these non-invertible zero-form symmetries can be broken by gauging the $\mathscr{G}_\mathbb{Z}$ subgroup of invertible symmetries.

hep-th

On the resolution of categorical symmetries in (Non-) Unitary Rational CFTs

We explore several aspects of categorical symmetry-resolved entanglement entropy (SREE) directly within two-dimensional rational conformal field theory (RCFT) (without invoking any SymTFT construction arXiv:2409.02806). We derive a general formula applicable whenever the action of the relevant topological defect lines on the annulus Hilbert space is known. This framework accommodates weakly and strongly symmetric boundaries, cloaking states, and fusion rings with multiplicities. We verify the formula in a range of diagonal unitary and non-unitary examples, including theories with generalized Haagerup-Izumi modular data. Furthermore, we extend the analysis to non-diagonal RCFTs. The $\frac{1}{2}E_6$ example demonstrates that closed-channel modular data and NIM-rep multiplicities alone do not suffice to determine the defect action on the complete open-channel Hilbert space.

hep-th

Reflecting boundary conditions in critical loop models

In critical loop models, we call a boundary sticky if loops can attach to it, and reflecting otherwise. Using analytic bootstrap methods, we show that reflecting boundaries are characterised by one complex parameter, analogous to the boundary cosmological constant in Liouville theory. We determine disc 1-point functions, and write an explicit formula for disc 2-point functions as infinite combinations of conformal blocks. We also sketch the lattice interpretation of reflecting boundaries.

hep-th