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In canonical LQG, unitarity is presumably guaranteed by the canonical formalism. How does one check for unitarity in the spin foam (path integral) formalism? Do the new spin foams pass the necessary tests?
marcus said:Unfortunately not available online, a talk given today at Princeton Institute for Advanced Studies:
Monday, April 23, 2012
High Energy Theory Seminar
“Loop Quantum Gravity: Recent Results and Open Problems”
Location: Bloomberg Lecture Hall
Time: 2:30 PM
Speaker(s): Carlo Rovelli, Centre de Physique Théorique de Luminy, Aix-Marseille University, France
Description: The loop approach to quantum gravity has developed considerably during the last few years, especially in its covariant ('spinfoam') version. I present the current definition of the theory and the results that have been proven. I discuss what I think is still missing towards of the goal of defining a consistent tentative quantum field theory genuinely background independent and having general relativity as classical limit.
http://www.princeton.edu/physics/events/viewevent.xml?id=347
negru said:I was at the talk at IAS, everyone was pretty confused by what he was doing. One point brought up was that there exist other models, like YM in 5d i think, whose discrete version has the correct classical limit and is uv and ir finite, but does not make sense quantum mechanically. And there was no concrete argument for why lqg would be a better example. Some numerical checks are needed, and he said they are very hard to do but people are working on them.
julian said:The Hamiltonian constraint operator in its usual form is non-hermitian, implying evolution is not unitary...but this is all OK because evolution with respect to the time coordinate has no physical meaning.
The reason it is non-Hermitian is that it only adds links at vertices but doesn't remove them.
atyy said:In canonical LQG, unitarity is presumably guaranteed by the canonical formalism. How does one check for unitarity in the spin foam (path integral) formalism? Do the new spin foams pass the necessary tests?
Unitarity in spin foams refers to the principle that the total probability of all possible outcomes of a quantum process must equal 1. In other words, the sum of all probabilities for a given event must equal 1, ensuring conservation of probability.
In Canonical LQG, unitarity is achieved through the use of a kinematical Hilbert space, which represents the space of all possible quantum states. The operators in this space must satisfy the unitarity condition, ensuring that the total probability of all possible states is conserved.
In Path Integrals, unitarity is achieved through the use of a sum-over-histories approach, where all possible paths of a quantum system are considered. The probabilities of these paths are then summed up, with the condition that the total probability must equal 1, ensuring unitarity.
The main difference is in their approach to unitarity. Canonical LQG uses a kinematical Hilbert space and operators satisfying the unitarity condition, while Path Integrals use a sum-over-histories approach to achieve unitarity.
Unitarity is important because it ensures the consistency of quantum processes and the conservation of probability. In spin foams, unitarity is necessary for the proper description of the dynamics of quantum spacetime, which is a key aspect of Canonical LQG and Path Integrals.