LQG vertex with finite Immirzi parameter

Abstract

We extend the definition of the "flipped" loop-quantum-gravity vertex to the case of a finite Immirzi parameter. We cover the Euclidean as well as the Lorentzian case. We show that the resulting dynamics is defined on a Hilbert space isomorphic to the one of loop quantum gravity, and that the area operator has the same discrete spectrum as in loop quantum gravity. This includes the correct dependence on the Immirzi parameter, and, remarkably, holds in the Lorentzian case as well. The ad hoc flip of the symplectic structure that was initially required to derive the flipped vertex is not anymore needed for finite Immirzi parameter. These results establish a bridge between canonical loop quantum gravity and the spinfoam formalism in four dimensions.

References in corpus (8)

• A new spinfoam vertex for quantum gravity
• The loop-quantum-gravity vertex-amplitude
• Flipped spinfoam vertex and loop gravity
• Linearized dynamics from the 4-simplex Regge action
• Spin foam model from canonical quantization
• The perturbative Regge-calculus regime of Loop Quantum Gravity
• Coherent states, constraint classes, and area operators in the new spin-foam models
• Numerical indications on the semiclassical limit of the flipped vertex

Cited by in corpus (7)

• Flipped spinfoam vertex and loop gravity
• The complete LQG propagator: II. Asymptotic behavior of the vertex
• Simplicity and closure constraints in spin foam models of gravity
• Coherent states, constraint classes, and area operators in the new spin-foam models
• Spin-Foam Models and the Physical Scalar Product
• Numerical indications on the semiclassical limit of the flipped vertex
• Tensorial Structure of the LQG graviton propagator