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Homework Statement
Working on an exercise from Srednicki's QFT and something is not clear.
Show that
[tex][\varphi(x), M^{uv}] = \mathcal{L}^{uv} \varphi(x)[/tex]
where
[tex]\mathcal{L}^{uv} = \frac{\hbar}{i} (x^u \partial^v - x^v \partial^u )[/tex]
Homework Equations
(1) [tex]U(\Lambda)^{-1} \varphi(x) U(\Lambda) = \varphi(\Lambda^{-1}x)[/tex]
(2) [tex]\Lambda = 1 + \delta\omega[/tex]
where [tex]\delta\omega [/itex] is an infinitesimal, and<br /> <br /> (3) [tex]U(\Lambda) = I + \frac{i}{2\hbar} \delta\omega_{uv} M^{uv}[/tex]<br /> <br /> <h2>The Attempt at a Solution</h2><br /> <br /> Got the left side of (1) equal to<br /> <br /> [tex]\varphi(x) + \frac{i}{2\hbar}\delta\omega_{uv}[\varphi(x), M^{uv}][/tex]<br /> <br /> but not sure what to do with the right side and how to get the desired derivatives. I suspect<br /> it has something to do with the transformation (1) of its derivative, but so far no luck.<br /> <br /> [tex]U(\Lambda)^{-1} \partial^u \varphi(x) U(\Lambda) = \Lambda^{u}_{ p} \bar{\partial}^p \varphi(\Lambda^{-1}x)[/tex][/tex]
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