Abstract
We explain how Feynman diagrams and the functional integral for quasi-Hermitian theories “know” about the metric η. The answer turns out be that their derivation is based fundamentally on the Heisenberg equations of motion and the canonical equal-time commutation relations, which only take their standard form when matrix elements are evaluated using η.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have