Introduction to Loop Quantum Gravity - Lecture 13: K=γL

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This course was given at the CPT in Marseille in February and March 2018. Lecture 13 is on an equation in the core of general relativity, which plays a major role in LQG.

(thanks to Pietropaolo Frisoni)
  1. CSTQ - Center for SpaceTime and the Quantum
  2. Carlo Rovelli
  3. LQG
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Комментарии
Автор

In minute 28 - why is the quantum theory affected by the (on-shell) boundary term we're adding to the classical action? One thought I have is that in the path integral it would manifestly make a difference, but is there an easy way to see this in the canonical formalism?

nicovaldes
Автор

Very few things actually exist. Have you ever thought of that? What are you going to do?

blitherbox