English

Invariant Connections in Loop Quantum Gravity

Mathematical Physics 2016-03-23 v2 General Relativity and Quantum Cosmology math.MP

Abstract

Given a group GG and an abelian CC^*-algebra A\mathfrak{A}, the antihomomorphisms Θ ⁣:GAut(A)\Theta\colon G\rightarrow \mathrm{Aut}(\mathfrak{A}) are in one-to-one with those left actions Φ ⁣:G×Spec(A)Spec(A)\Phi\colon G\times \mathrm{Spec}(\mathfrak{A})\rightarrow \mathrm{Spec}(\mathfrak{A}) whose translation maps Φg\Phi_g are continuous; whereby continuities of Θ\Theta and Φ\Phi turn out to be equivalent if A\mathfrak{A} is unital. In particular, a left action ϕ ⁣:G×XX\phi\colon G \times X\rightarrow X can be uniquely extended to the spectrum of a CC^*-subalgebra A\mathfrak{A} of the bounded functions on XX if ϕg(A)A\phi_g^*(\mathfrak{A})\subseteq \mathfrak{A} holds for each gGg\in G. In the present paper, we apply this to the framework of loop quantum gravity. We show that, on the level of the configuration spaces, quantization and reduction in general do not commute, i.e., that the symmetry-reduced quantum configuration space is (strictly) larger than the quantized configuration space of the reduced classical theory. Here, the quantum-reduced space has the advantage to be completely characterized by a simple algebraic relation, whereby the quantized reduced classical space is usually hard to compute.

Keywords

Cite

@article{arxiv.1307.5303,
  title  = {Invariant Connections in Loop Quantum Gravity},
  author = {Maximilian Hanusch},
  journal= {arXiv preprint arXiv:1307.5303},
  year   = {2016}
}

Comments

33 pages. Revised version: Proof of Theorem 4.8 simplified; comments added to Sect. 1 and Sect. 5

R2 v1 2026-06-22T00:54:31.175Z