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Quantized Curvature in Loop Quantum Gravity

Mathematical Physics 2019-02-20 v1 math.MP

Abstract

A hyperlink is a finite set of non-intersecting simple closed curves in R×R3\mathbb{R} \times \mathbb{R}^3. Let SS be an orientable surface in R×R3\mathbb{R} \times \mathbb{R}^3. The Einstein-Hilbert action S(e,ω)S(e,\omega) is defined on the vierbein ee and a su(2)×su(2)\mathfrak{su}(2)\times\mathfrak{su}(2)-valued connection ω\omega, which are the dynamical variables in General Relativity. Define a functional FS(ω)F_S(\omega), by integrating the curvature dω+ωωd\omega + \omega \wedge \omega over the surface SS, which is su(2)×su(2)\mathfrak{su}(2)\times\mathfrak{su}(2)-valued. We integrate FS(ω)F_S(\omega) against a holonomy operator of a hyperlink LL, disjoint from SS, and the exponential of the Einstein-Hilbert action, over the space of vierbeins ee and su(2)×su(2)\mathfrak{su}(2)\times\mathfrak{su}(2)-valued connections ω\omega. Using our earlier work done on Chern-Simons path integrals in R3\mathbb{R}^3, we will write this infinite dimensional path integral as the limit of a sequence of Chern-Simons integrals. Our main result shows that the quantized curvature can be computed from the linking number between LL and SS.

Keywords

Cite

@article{arxiv.1803.01310,
  title  = {Quantized Curvature in Loop Quantum Gravity},
  author = {Adrian P. C. Lim},
  journal= {arXiv preprint arXiv:1803.01310},
  year   = {2019}
}

Comments

arXiv admin note: text overlap with arXiv:1705.06577, arXiv:1706.01011, arXiv:1705.00396

R2 v1 2026-06-23T00:41:19.135Z