1994/12/05 by Abhay Ashtekar, Jerzy Lewandowski, Donald Marolf +2
Physics and Astronomy · #gr-qc #hep-th
published as J.Funct.Anal. 135 (1996) 519-551 · 38 pages, latex
arxiv created 1994/12/05 · arxiv updated 2009/11/30
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 μH, the Hall transform is an isometric isomorphism from L2(G, μH) to \cal H(G\Co)∩ L2(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^⋆ 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.