The electromagnetic stress tensor Fμν is as we all know traceless in 4 dimensions. With Fμν=∂μAν−∂νAμ and A=(A0,A1,A2,A3)=(ϕ,A1,A2,A3)
In other dimensions this is not the case? If so how does one expand either the definition of Fμν and A?
Edit: I was clearly wrong with the with terminology, I meant the electromagnetic stress-energy tensor (or electromagnetic energy-momentum tensor) which was pointed out in the comment section.
No comments:
Post a Comment