2005
DOI: 10.1590/s0103-97332005000300019
|View full text |Cite
|
Sign up to set email alerts
|

The Feynman propagator for quantum gravity: spin foams, proper time, orientation, causality and timeless-ordering

Abstract: We discuss the notion of causality in Quantum Gravity in the context of sum-over-histories approaches, in the absence therefore of any background time parameter. In the spin foam formulation of Quantum Gravity, we identify the appropriate causal structure in the orientation of the spin foam 2-complex and the data that characterize it; we construct a generalised version of spin foam models introducing an extra variable with the interpretation of proper time and show that different ranges of integration for this… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
5
0

Year Published

2006
2006
2022
2022

Publication Types

Select...
6
1

Relationship

0
7

Authors

Journals

citations
Cited by 7 publications
(5 citation statements)
references
References 16 publications
0
5
0
Order By: Relevance
“…Furthermore the Ponzano Regge model includes in addition also a sum over orientations, which we do not consider here. The question arises, whether this result can be extended to the full non-linear theory and shed light on the problem, whether to include a sum over orientations into a quantum gravity path integral or not [57,58].…”
Section: Discussionmentioning
confidence: 99%
“…Furthermore the Ponzano Regge model includes in addition also a sum over orientations, which we do not consider here. The question arises, whether this result can be extended to the full non-linear theory and shed light on the problem, whether to include a sum over orientations into a quantum gravity path integral or not [57,58].…”
Section: Discussionmentioning
confidence: 99%
“…Nevertheless, there is good evidence that the transition amplitudes for semiclassical states 29 are able to select dynamically the globally oriented configurations (see [51] for a comprehensive discussion in the context of Regge calculus and [57] for a single-vertex discussion in spinfoams). In the Lorentzian setting, the definition of causal amplitudes makes use of modified spinfoam amplitudes which are orientation-dependent [58][59][60].…”
Section: Discussionmentioning
confidence: 99%
“…This amounts to dropping one SL(2, C) integral per each vertex.The map Y is constructed using the principal series of unitary representations H (j,ρ) of SL(2, C), which are infinite dimensional and labeled by a half-integer j and a positive real number ρ. The spinfoam model imposes the constraint ρ = γk(59)…”
mentioning
confidence: 99%
“…Further investigation is still necessary to better understand the issue and how it is related to the imposition of constraints in the spin-foam path integral. We would however be remiss in not pointing out that the Cosine Problem's existence has been associated to a time-orientation symmetry in spin-foam models: in [52,53] the point is made that a causal ordering for spin-foams may be enforced by making the amplitudes explicitly dependent on the orientation of the geometry, thus breaking time reversal symmetry. As we have shown, spin-foam vertices with mixed causal characters induce a second solution if one transforms the boundary data appropriately.…”
Section: Discussion and Outlookmentioning
confidence: 99%