Robert Mann - An Introduction to Particle Physics and the Standard Model · Problem 11.6.4

Quantum Electrodynamics — Robert Mann

Physics — Particle Physics · gamma-matrix-trace-identities

Problem

Prove the following: Tr[I]=4andTr[γμγν]=4gμν\mathrm{Tr}[I] = 4 \quad \text{and} \quad \mathrm{Tr}[\gamma^\mu\gamma^\nu] = 4g^{\mu\nu} Tr[odd # of γ-matrices]=0\mathrm{Tr}[\text{odd }\# \text{ of }\gamma\text{-matrices}] = 0 Tr[γμγνγαγβ]=4(gμνgαβ−gμαgνβ+gμβgνα)\mathrm{Tr}[\gamma^\mu\gamma^\nu\gamma^\alpha\gamma^\beta] = 4\left(g^{\mu\nu}g^{\alpha\beta} - g^{\mu\alpha}g^{\nu\beta} + g^{\mu\beta}g^{\nu\alpha}\right) Tr[γ5γμγνγαγβ]=−4iεμναβwithε0123=−1\mathrm{Tr}[\gamma^5\gamma^\mu\gamma^\nu\gamma^\alpha\gamma^\beta] = -4i\varepsilon^{\mu\nu\alpha\beta} \quad \text{with} \quad \varepsilon^{0123} = -1 γαγνγα=−2γν\gamma_\alpha\gamma^\nu\gamma^\alpha = -2\gamma^\nu γαγμγνγα=4gμν\gamma_\alpha\gamma^\mu\gamma^\nu\gamma^\alpha = 4g^{\mu\nu} Tr[γ5]=0\mathrm{Tr}[\gamma^5] = 0 where εμναβ\varepsilon^{\mu\nu\alpha\beta} is the 4-dimensional Levi-Civita symbol (or epsilon-tensor) which obeys ε0123=−1ε0123=+1\varepsilon^{0123} = -1 \qquad \varepsilon_{0123} = +1 εμναβ={−1(if μναβ is an even permutation of 0123)+1(if μναβ is an odd permutation of 0123)\varepsilon^{\mu\nu\alpha\beta} = \begin{cases} -1 & (\text{if }\mu\nu\alpha\beta\text{ is an even permutation of }0123) \\ +1 & (\text{if }\mu\nu\alpha\beta\text{ is an odd permutation of }0123) \end{cases} εμναβ={+1(if μναβ is an even permutation of 0123)−1(if μναβ is an odd permutation of 0123)\varepsilon_{\mu\nu\alpha\beta} = \begin{cases} +1 & (\text{if }\mu\nu\alpha\beta\text{ is an even permutation of }0123) \\ -1 & (\text{if }\mu\nu\alpha\beta\text{ is an odd permutation of }0123) \end{cases}

Related theory

Browse the problem library