Manuscript Oai282-A@1 · Oai282-A.tex · section · 5b6134ec

The reported framework

Stage 0: the Family 282 statement as a source record › The reported framework · lines 249–317

Oai282-A@1#record:main, Oai282-A@1#eq:record-improvement

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The supplied :framework concerns an already specified theory on

Its reported inputs include:

  1. a local unitary positive-energy vacuum representation, with a Poincaré- and scale-invariant vacuum;

  2. an original physical field-label space

    with discrete, bounded-below, locally finite scaling grades and finite Lorentz multiplicities;

  3. finite scaling support for every original field;

  4. compatible realizations of the original fields and their adjoints affiliated with a fixed covariant causally commuting bounded local net;

  5. a physical local dilatation current implementing scale transformations through its local Ward identities;

  6. the source's original-product, domain, and physical-field admission conventions.

The reported assumptions do not separately impose uniqueness of the invariant vector, Haag duality, the split property, a phase-space estimate, or field-operator energy bounds OpenAI282,Dossier. This list is a scoped account of the supplied framework, not a replacement for every clause of the original assumption.

Under its full :framework, the supplied preprint claims that the physical stress tensor has a symmetric conserved traceless local improvement with unchanged translation and Lorentz Ward charges.

After selecting Hermitian dimension-four and dimension-three components and , it claims a Hermitian physical scalar of dimension two satisfying

such that

is symmetric, conserved, and traceless. It further claims unbroken local Ward identities for , for conformal Killing fields .

The conclusion is local. Integration to a global conformal action on the whole bounded net is left as a separate question OpenAI282,Dossier.

The source claims to derive the scalar condition from a more general improvement problem, rather than assuming it. Our conditional calculations below do not reproduce that derivation.

Displayed formulas in this passage

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