A. Zee, Quantum Field Theory in a Nutshell · Problem VIII.1.8

Field Theory Redux

Physics — QFT

Problem

The vielbeins for a spacetime with Minkowski metric is defined by gμν(x)=eaμ(x)ηabebν(x)g_{\mu\nu}(x) = e^a{}_\mu(x)\eta_{ab}e^b{}_\nu(x), where the Minkowski metric ηab\eta_{ab} replaces the Euclidean metric δab\delta_{ab}. The indices aa and bb are to be contracted with ηab\eta_{ab}. For example, Rab=dωab+ωacηcdωdbR^{ab} = d\omega^{ab} + \omega^a{}_c\eta^{cd}\omega_d{}^b. Show that everything goes through as expected.

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