= Improved stress-energy tensor of a free massless scalar
{title2=$\Theta_{\mu\nu}=\partial_\mu\phi\partial_\nu\phi-\frac12\eta_{\mu\nu}(\partial\phi)^2+\frac{d-2}{4(d-1)}(\eta_{\mu\nu}\Box-\partial_\mu\partial_\nu)\phi^2$}
For $d>1$, the displayed <stress-energy tensor> is symmetric and conserved on the free massless <scalar field> equation $\Box\phi=0$. Its improvement is identically divergence-free. Since $\Box\phi^2=2(\partial\phi)^2$ on shell, its trace vanishes. Contracting it with a <Conformal Killing vector field> therefore produces a conserved conformal current. In $d=2$ the improvement coefficient is zero: the canonical tensor already has zero trace.
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