Introduction to Loop Quantum Gravity - Lecture 14: Again K=γL.

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This course was given at the CPT in Marseille in February and March 2018. Lecture 14 is on several geometric and physical aspects of the equation K=γL.

(thanks to Pietropaolo Frisoni)
  1. CSTQ - Center for SpaceTime and the Quantum
  2. Carlo Rovelli
  3. LQG
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Thank you for amazing lecture series. I've cordially enjoyed it!


It might be too late to ask, but I'm very much confused about appearance of "gamma" in the area operator. The surface area has to be an integral over a 2-form (pull-back of the volume form to the surface) and my calculations show that it has to be just "1/2 \epsilon_{IJ} e^I \wedge e^J" given that we have a restriction of triad to the surface "e^I". How does "gamma" enter this calculation?

Theo