physlad
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I was reading about the momentum-energy tensor (or stress-energy tensor), at one point the author says,
"
\theta^{\mu\nu} = (\partial^\mu\phi)(\partial^\nu\phi) - g^{\mu\nu}L
This is clearly symmetric in \mu and \nu."
\theta^{\mu\nu}: is the stress-energy tensor
\phi is a scalar field
g^{\mu\nu} is the metric (+---)
L is the lagrangian density
My question (I'm not an expert in tensors) is how do you see that it's "clearly" symmetric? another silly question: when do we need to symmetrize and antisymmetrize tensors?
Please, tell me guys if this isn't the right place for my question.
"
\theta^{\mu\nu} = (\partial^\mu\phi)(\partial^\nu\phi) - g^{\mu\nu}L
This is clearly symmetric in \mu and \nu."
\theta^{\mu\nu}: is the stress-energy tensor
\phi is a scalar field
g^{\mu\nu} is the metric (+---)
L is the lagrangian density
My question (I'm not an expert in tensors) is how do you see that it's "clearly" symmetric? another silly question: when do we need to symmetrize and antisymmetrize tensors?
Please, tell me guys if this isn't the right place for my question.