The stress tensor for a conformal field theory (or any quantum field theory) can be derived from the action S by the functional derivative
Tμν = −2√|g|δSδgμν,
where gμν is the background metric of signature (+,−,−,−). This formula for the stress tensor appears to be identically symmetric, i.e. Tμν=Tνμ
for any field configuration in the path integral, not just those obeying the classical equations of motion.
On the other hand, I don't see how this is consistent with the Ward identity (e.g. see Di Francesco et al, p. 107)
⟨(Tμν−Tνμ)X⟩ = −i∑iδ(x−xi)Sνμi⟨X⟩,
where X is some product of fields ϕ(x1)⋯ϕ(xn), and the field ϕ transforms internally under an infinitesimal rotation xμ→xμ+ωμνxν as ϕ→ϕ+ωμνSμνϕ.
If Tμν was identically symmetric, then both sides should equal zero.
This post imported from StackExchange Physics at 2015-05-04 13:53 (UTC), posted by SE-user Dominic Else