- #1
waht
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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
(3) [tex] U(\Lambda) = I + \frac{i}{2\hbar} \delta\omega_{uv} M^{uv} [/tex]
The Attempt at a Solution
Got the left side of (1) equal to
[tex] \varphi(x) + \frac{i}{2\hbar}\delta\omega_{uv}[\varphi(x), M^{uv}] [/tex]
but not sure what to do with the right side and how to get the desired derivatives. I suspect
it has something to do with the transformation (1) of its derivative, but so far no luck.
[tex] U(\Lambda)^{-1} \partial^u \varphi(x) U(\Lambda) = \Lambda^{u}_{ p} \bar{\partial}^p \varphi(\Lambda^{-1}x) [/tex]
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