Noether current in quantum field theory

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The discussion revolves around deriving the Noether current for a specific action involving a 2x2 matrix field under a transformation. The infinitesimal transformation has been identified as δα = [α, φ], where α and φ are real 2x2 matrices. The challenge lies in calculating the Noether current, particularly the covariant derivatives due to the matrix nature of φ. The user seeks assistance in applying the Noether current formula, specifically how to handle the matrix elements in the derivatives. The conversation highlights the complexity of working with matrix fields in quantum field theory.
CSpring432
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Homework Statement
Finding Noether current for the given action
Relevant Equations
$$J^{\mu}=\frac{\partial L(\phi, \partial (\phi))}{\partial (\partial _{\mu}(\phi)}(\delta_{\alpha}\phi)-F^{\mu}$$
Hi

Have been trying to solve the below question for a while, wondered if anyone could help.

Considering the action

$$S=\int -\frac{1}{2}\sum^2_{n,m=1} (\partial^{\mu}\phi_{nm}\partial_{\mu}\phi_{mn}+m^2 \phi_{nm} \phi_{mn})dx$$
under the transformation

$$\phi'=e^{\alpha}\phi e^{-\alpha}$$

Find the infinitesimal transformation and associated Noether current, where both ##\alpha## and ##\phi## are real 2x2 matrices.

I've managed to find what (I think) is the infinitesimal transformation:

$$e^{\alpha}\phi e^{-\alpha}\approx \phi-\phi \alpha +\alpha\phi+ \mathcal{O}(\alpha^2)$$
$$\therefore \delta_{\alpha}=[\alpha, \phi]$$

I am however, stumped for calculating the Noether constant. I know that I would have to use the formula

$$J^{\mu}=\frac{\partial L(\phi, \partial (\phi))}{\partial (\partial _{\mu}(\phi)}(\delta_{\alpha}\phi)-F^{\mu}$$

The issue, I think, is calculating the covariant derivatives since the phi terms are matrix elements. Any help would be really appreciated.
 
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I think that ##\phi## represents four real fields ##\phi_{nm}## and the first term in the Noether current is
$$\sum^2_{n,m=1}\frac{\partial L(\phi, \partial (\phi))}{\partial (\partial _{\mu}(\phi_{nm}))}(\delta_{\alpha}\phi_{nm})$$
 
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