1996/12/12 by Giorgio Immirzi · 13 citations
Physics and Astronomy · #Black Holes and Theoretical Physics #Canonical quantization #Canonical quantum gravity #Connection (principal bundle) #Cosmology and Gravitation Theories #Gauge (firearms) #Gauge theory #Hamiltonian (control theory) #Noncommutative and Quantum Gravity Theories #Poisson bracket #Quantum #Quantum gravity #gr-qc
paper · pdf · doi:10.1088/0264-9381/14/10/002
published as Class.Quant.Grav.14:L177-L181,1997 · 8 pages, RevTeX, no figures
arxiv created 1996/12/12 · openalex publication_date 1997/10/01 · arxiv updated 2010/04/06 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/06
Both real and complex connections have been used for canonical gravity: the complex connection has SL(2,C) as the gauge group, while the real connection has SU(2) as the gauge group. We show that there is an arbitrary parameter which enters in the definition of the real connection, in the Poisson brackets, and therefore in the scale of the discrete spectra one finds for areas and volumes in the corresponding quantum theory. A value for could be singled out in the quantum theory by the Hamiltonian constraint or by the rotation to the complex Ashtekar connection.