TriTertButoxy
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I have a simple technical problem. I'm following a paper [Shore, G. Ann Phys. 137, 262-305 (1981)], and I am unable to show a very simple identity for the non-abelian fluctuation operator (eq 4.37):
where \phi is a test function and (F_{\mu\nu})^{ab}\equiv gf^{abc}F_{\mu\nu}^{c}=[D_\mu,\,D_\nu], and hence D_\mu F_{\mu\nu}=D^2D_\nu-D_\mu D_\nu D_\mu (color indices suppressed). So far, I have worked on the LHS, and I'm almost there:
\text{LHS}=(-D_\nu D^2+D^2 D_\nu-2D_\mu F_{\mu\nu})\phi[/itex]<br /> \phantom{LHS}=(-\underline{D_\mu D_\nu D_\mu}-[D_\nu,\,D_\mu]D_\mu+\underline{D^2D_\nu}-2D_\mu F_{\mu\nu})\phi<br /> combine underlined terms using identity stated above<br /> =(-[D_\nu,\,D_\mu]D_\mu+D_\mu F_{\mu\nu}-2D_\mu F_{\mu\nu})\phi<br /> then first term is -[D_\nu,\,D_\mu]D_\mu=+F_{\mu\nu}D_\mu, and 2nd and 3rd terms add<br /> =(F_{\mu\nu}D_\mu-D_\mu F_{\mu\nu})\phi<br /> Finally, use product rule in 2nd term: D_\mu(fg)=(D_\mu f)g+f\partial_\mu g.<br /> =F_{\mu\nu}(\partial+A)_\mu\phi-(D_\mu F_{\mu\nu})\phi-F_{\mu\nu}\,\partial_\mu\phi<br /> to get<br /> =F_{\mu\nu} A_\mu \phi-(D_\mu F_{\mu\nu})\phi.<br /> <br /> This is <i>almost</i> equal to RHS, except for that stupid A_\mu term. How the hell do I get rid of it?!?
D_\mu\left[-D^2\delta_{\mu\nu}+D_\mu D_\nu-2F_{\mu\nu}\right]\,\phi=-(D_\mu F_{\mu\nu})\,\phi , (typo fixed)
where \phi is a test function and (F_{\mu\nu})^{ab}\equiv gf^{abc}F_{\mu\nu}^{c}=[D_\mu,\,D_\nu], and hence D_\mu F_{\mu\nu}=D^2D_\nu-D_\mu D_\nu D_\mu (color indices suppressed). So far, I have worked on the LHS, and I'm almost there:
\text{LHS}=(-D_\nu D^2+D^2 D_\nu-2D_\mu F_{\mu\nu})\phi[/itex]<br /> \phantom{LHS}=(-\underline{D_\mu D_\nu D_\mu}-[D_\nu,\,D_\mu]D_\mu+\underline{D^2D_\nu}-2D_\mu F_{\mu\nu})\phi<br /> combine underlined terms using identity stated above<br /> =(-[D_\nu,\,D_\mu]D_\mu+D_\mu F_{\mu\nu}-2D_\mu F_{\mu\nu})\phi<br /> then first term is -[D_\nu,\,D_\mu]D_\mu=+F_{\mu\nu}D_\mu, and 2nd and 3rd terms add<br /> =(F_{\mu\nu}D_\mu-D_\mu F_{\mu\nu})\phi<br /> Finally, use product rule in 2nd term: D_\mu(fg)=(D_\mu f)g+f\partial_\mu g.<br /> =F_{\mu\nu}(\partial+A)_\mu\phi-(D_\mu F_{\mu\nu})\phi-F_{\mu\nu}\,\partial_\mu\phi<br /> to get<br /> =F_{\mu\nu} A_\mu \phi-(D_\mu F_{\mu\nu})\phi.<br /> <br /> This is <i>almost</i> equal to RHS, except for that stupid A_\mu term. How the hell do I get rid of it?!?
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