I have a problem providing or finding a general proof for this statement i found in Mussardo's statistical field theory book, section $10.3.2$:
Due to the locality of the theory there exists a local field $T_{\mu\nu}(x)$, called the stress-energy tensor, defined by the variation of the local action $S[\varphi]$ under the infinitesimal transformation $x^{\,\mu} \rightarrow x^{' \mu} = x^{\,\mu} + \epsilon^{\,\mu}(x)$
$$ \delta S \, =\, \frac{1}{(2 \pi)^{D-1}} \int d^Dx \, T_{\mu\nu}(x)\, \partial^{\,\mu} \epsilon^{\,\nu} $$
where it says that the factor $(2 \pi)^{D-1}$ is there for later convenience
Now I've seen the proof for a real scalar field which is clearly a field without local interactions.
What is the proof in the general case? Is there a place (book or article) where I can find the proof?