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kalish
Apr20-11, 03:09 PM
Hi, I am currently in training and while deriving the EOM for a specific lagrangian I am having difficulties to prove thatg^{\mu \nu} \delta R_{\mu \nu} B(\phi) = (\nabla_{\mu} \nabla_\nu - \square B g_\mu_\nu) I am ashamed it might be a simple calculus but I don't see how. If you had just hints to help me that would be fair.

Moreover I would like to check wether \square = \frac{\partial_\mu (\sqrt{-g}g^\mu^\nu)\partial_\nu}{\sqrt{-g}} as I found or \square = \frac{\partial_\mu\sqrt{-g}g^\mu^\nu\partial_\nu}{\sqrt{-g}} as I read into one reference.


Thanks.

kalish
Apr20-11, 03:14 PM
well latex doesn't semm to work pretty well with me...

Bill_K
Apr20-11, 04:59 PM
◻Φ = (1/√-g)(∂μ(√-g gμν ∂νΦ))

kalish
Apr21-11, 02:40 AM
thanks.
But the more important was how I can prove the first equation about the riemann tensor.

it lacks a\delta g{\mu \nu} on the right member of the first equation. But however I think I can manage now.

and you should read (\nabla_\mu \nabla_\nu -g_{\mu\nu}\square)B

but I found it