Coherent State Transforms for Spaces of Connections
| dc.creator | Ashtekar, Abhay | |
| dc.creator | Lewandowski, Jerzy | |
| dc.creator | Marolf, Donald | |
| dc.creator | Mourão, José | |
| dc.creator | Thiemann, Thomas | |
| dc.date | 1994-12-05 | |
| dc.date.accessioned | 2026-07-07T03:30:34Z | |
| dc.date.available | 2026-07-07T03:30:34Z | |
| dc.description | The Segal-Bargmann transform plays an important role in quantum theories of linear fields. Recently, Hall obtained a non-linear analog of this transform for quantum mechanics on Lie groups. Given a compact, connected Lie group $G$ with its normalized Haar measure $μ_H$, the Hall transform is an isometric isomorphism from $L^2(G, μ_H)$ to ${\cal H}(G^{\Co})\cap L^2(G^{\Co}, ν)$, where $G^{\Co}$ the complexification of $G$, ${\cal H}(G^{\Co})$ the space of holomorphic functions on $G^{\Co}$, and $ν$ an appropriate heat-kernel measure on $G^{\Co}$. We extend the Hall transform to the infinite dimensional context of non-Abelian gauge theories by replacing the Lie group $G$ by (a certain extension of) the space ${\cal A}/{\cal G}$ of connections modulo gauge transformations. The resulting ``coherent state transform'' provides a holomorphic representation of the holonomy $C^\star$ algebra of real gauge fields. This representation is expected to play a key role in a non-perturbative, canonical approach to quantum gravity in 4-dimensions. | |
| dc.description | 38 pages, latex | |
| dc.identifier | https://arxiv.org/abs/gr-qc/9412014 | |
| dc.identifier | http://arxiv.org/abs/gr-qc/9412014 | |
| dc.identifier | J.Funct.Anal. 135 (1996) 519-551 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/35566 | |
| dc.subject | General Relativity and Quantum Cosmology | |
| dc.subject | High Energy Physics - Theory | |
| dc.title | Coherent State Transforms for Spaces of Connections | |
| dc.type | text |