English

Geometric foundations for classical $\mathrm{U}(1)$-gauge theory on noncommutative manifolds

Mathematical Physics 2024-08-26 v2 High Energy Physics - Theory math.MP Operator Algebras Quantum Algebra

Abstract

We systematically extend the elementary differential and Riemannian geometry of classical U(1)\mathrm{U}(1)-gauge theory to the noncommutative setting by combining recent advances in noncommutative Riemannian geometry with the theory of coherent 22-groups. We show that Hermitian line bimodules with Hermitian bimodule connection over a unital pre-C\mathrm{C}^\ast-algebra with \ast-exterior algebra form a coherent 22-group, and we prove that weak monoidal functors between coherent 22-groups canonically define bar or involutive monoidal functors in the sense of Beggs--Majid and Egger, respectively. Hence, we prove that a suitable Hermitian line bimodule with Hermitian bimodule connection yields an essentially unique differentiable quantum principal U(1)\mathrm{U}(1)-bundle with principal connection and vice versa; here, U(1)\mathrm{U}(1) is qq-deformed for qq a numerical invariant of the bimodule connection. From there, we formulate and solve the interrelated lifting problems for noncommutative Riemannian structure in terms of abstract Hodge star operators and formal spectral triples, respectively; all the while, we account precisely for emergent modular phenomena of geometric nature. In particular, it follows that the spin Dirac spectral triple on quantum CP1\mathbf{C}\mathrm{P}^1 does not lift to a twisted spectral triple on 33-dimensional quantum SU(2)\mathrm{SU}(2) with the 33-dimensional calculus but does recover Kaad--Kyed's compact quantum metric space on quantum SU(2)\mathrm{SU}(2) for a canonical choice of parameters.

Keywords

Cite

@article{arxiv.2301.01749,
  title  = {Geometric foundations for classical $\mathrm{U}(1)$-gauge theory on noncommutative manifolds},
  author = {Branimir Ćaćić},
  journal= {arXiv preprint arXiv:2301.01749},
  year   = {2024}
}

Comments

85 pp. Minor revision for submission. The material originally in Section 4.1 on Hodge decomposition and Maxwell's equations has been set aside for future work

R2 v1 2026-06-28T08:02:53.588Z