Contraction in the Riemann Tensor

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Fraser
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Hi all,

I'm trying to follow through some of my notes of a GR course. The notes are working towards a specific expression and the following line appears:

[tex]R^{\alpha \beta}_{\gamma \delta ; \mu} + R^{\alpha \beta}_{\delta \mu ; \gamma} + R^{\alpha \beta}_{\mu \gamma ; \delta}=0[/tex]

Which by contraction over [tex]\alpha[/tex] and [tex]\gamma[/tex] becomes

[tex]R^{\alpha \beta}_{\alpha\delta ; \mu} + R^{\alpha \beta}_{\delta \mu ; \alpha} + R^{\alpha \beta}_{\mu \alpha; \delta}=0[/tex]

I'm afraid I don't understand this, it seems to relabel [tex]\gamma[/tex] with[tex]\alpha[/tex]. But how can we do this?

I do understand contraction in general, such that for a general tensor

[tex]T^{\alpha}_{\beta}=T^{\rho \alpha }_{\beta \rho}[/tex]

But I don't see how this has been applied here?

Thanks in advance

p.s If this is more of a general maths question then please move to the appropriate forum
 
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From your first equation,

[tex] \delta^\gamma_\alpha \left( R^{\alpha \beta}_{\gamma \delta ; \mu} + R^{\alpha \beta}_{\delta \mu ; \gamma} + R^{\alpha \beta}_{\mu \gamma ; \delta} \right)=0[/tex]

Now do the sum over [itex]\gamma[/itex].
 
Wow, thank you! 4 of us working together didn't think of that :(