Physics Asked on July 19, 2021
I want to show that tr($gamma^mu gamma^nu$) = 4$eta^{mu nu}$.
I know that {$gamma^mu , gamma^nu$} = 2$eta^{munu}I_4$ and tr($gamma^mu gamma^nu$) = tr($gamma^nu gamma^mu$),
so tr($gamma^mu gamma^nu$) = tr(2$eta^{munu} I_4$ – $gamma^nu gamma^mu$) $implies$ 2tr($gamma^mu gamma^nu$) = 2tr($eta^{munu} I_4$), and ony way to get the answer is by pulling out $eta^{munu}$ out of the trace.
I want to ask how we can do that? since $eta^{munu}$ is itself a matrix, then why it is taken out of the trace and its diagonal elements are not summed?
The trace is over the matrix indices which represent the internal degrees of freedom of the spinor, not over the space-time indices.
Each $gamma^mu$ is a matrix, so if we want to write out all the indices explicitely, it would be $(gamma^mu)^{i}_{~~j}$. Then ${gamma^nu,gamma^mu} = 2eta^{munu}$ becomes : $$(gamma^mu)^i_{~~j}(gamma^{nu})^j_{~~k} + (gamma^nu)^i_{~~j}(gamma^{mu})^j_{~~k} = 2 eta^{munu}delta^i_k$$
and what you want to show is : $$(gamma^mu)^i_{~~j}(gamma^nu)^j_{~~i} = 2 eta^{munu}$$
So the short answer is : the $eta^{munu}$ goes out of the trace freely.
Correct answer by SolubleFish on July 19, 2021
Get help from others!
Recent Questions
Recent Answers
© 2024 TransWikia.com. All rights reserved. Sites we Love: PCI Database, UKBizDB, Menu Kuliner, Sharing RPP