Canonical T^{μν} = (∂ℒ/∂(∂_μ φ)) ∂^ν φ − η^{μν} ℒ; conserved by translation invariance (Noether). Belinfante–Rosenfeld improvement makes it symmetric.
Canonical T^{μν} = (∂ℒ/∂(∂_μ φ)) ∂^ν φ − η^{μν} ℒ; conserved by translation invariance (Noether). Belinfante–Rosenfeld improvement makes it symmetric.