mathematical-physics / Axiomatic quantum field theory: scale and conformal symmetry

Scale invariance implies local conformal invariance for a class of four-dimensional unitary QFTs

Theorem 1.1: under the paper's framework (unitary, positive energy, Poincare- and scale-invariant vacuum, discrete bounded-below dimension spectrum with finite multiplicities, finite scaling support, bounded local net, physical stress tensor and virial current), there is a Hermitian dimension-two physical scalar LL with ∂μVμ(3)=□L\partial^\mu V^{(3)}_\mu=\Box L, so Tμν(4)+13(∂μ∂ν−ημν□)LT^{(4)}_{\mu\nu}+\tfrac13(\partial_\mu\partial_\nu-\eta_{\mu\nu}\Box)L is symmetric, conserved and traceless with unchanged translation and Lorentz charges, and conformal currents have unbroken local Ward identities. It does not treat theories outside these hypotheses (continuous spectra, no bounded net, no local virial current), and integration to a global conformal action on the net is left open.

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mathematical-physicsSep 26, 2026Significance 30/100Registry: unreviewed

Scale invariance implies local conformal invariance for a class of four-dimensional unitary QFTs

Prior state unknown→proved

Theorem 1.1: under the paper's framework (unitary, positive energy, Poincare- and scale-invariant vacuum, discrete bounded-below dimension spectrum with finite multiplicities, finite scaling support, bounded local net, physical stress tensor and virial current), there is a Hermitian dimension-two physical scalar LL with ∂μVμ(3)=□L\partial^\mu V^{(3)}_\mu=\Box L, so…

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Theorem 1.1: under the paper's framework (unitary, positive energy, Poincare- and scale-invariant vacuum, discrete bounded-below dimension spectrum with finite multiplicities, finite scaling support, bounded local net, physical stress tensor and virial current), there is a Hermitian dimension-two physical scalar LL with ∂μVμ(3)=□L\partial^\mu V^{(3)}_\mu=\Box L, so Tμν(4)+13(∂μ∂ν−ημν□)LT^{(4)}_{\mu\nu}+\tfrac13(\partial_\mu\partial_\nu-\eta_{\mu\nu}\Box)L is symmetric, conserved and traceless with unchanged translation and Lorentz charges, and conformal currents have unbroken local Ward identities. It does not treat theories outside these hypotheses (continuous spectra, no bounded net, no local virial current), and integration to a global conformal action on the net is left open.

Theorem 1.1: under the paper's framework (unitary, positive energy, Poincare- and scale-invariant vacuum, discrete bounded-below dimension spectrum with finite multiplicities, finite scaling support, bounded local net, physical stress tensor and virial current), there is a Hermitian dimension-two physical scalar LL with ∂μVμ(3)=□L\partial^\mu V^{(3)}_\mu=\Box L, so Tμν(4)+13(∂μ∂ν−ημν□)LT^{(4)}_{\mu\nu}+\tfrac13(\partial_\mu\partial_\nu-\eta_{\mu\nu}\Box)L is symmetric, conserved and traceless with unchanged translation and Lorentz charges, and conformal currents have unbroken local Ward identities. It does not treat theories outside these hypotheses (continuous spectra, no bounded net, no local virial current), and integration to a global conformal action on the net is left open.

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