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Feb 2, 2014 at 6:58 comment added Ruslan @gj255 indeed, I didn't see the obvious possibility to lower the indices on the RHS and get the simple relation. Have to do more index gymnastics to get used to it :)
Feb 1, 2014 at 20:19 vote accept Ruslan
Feb 1, 2014 at 19:23 answer added Valter Moretti timeline score: 1
Feb 1, 2014 at 13:12 comment added gj255 The vector on the RHS may involve contravariant components of the 4-momentum, but it is certainly not equal to $$ (p^0,p^1,p^2,p^3) \,,$$ which are the contravariant components of the 4-momentum. Using the relation $$p_\mu = \eta_{\mu \nu} p^\nu $$ we see that the list of components on the right are indeed the covariant components of the 4-momentum. The covariant and contravariant components of an object are closely related, and so it is natural that we could write them in terms of each other --- we have $p_1 = -p^1$, for instance.
Feb 1, 2014 at 13:02 history asked Ruslan CC BY-SA 3.0