Gauge-dressed theorem and actual link action.
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The bare theorem above makes no Gauss-sector claim. For the [formula in source] analogue and [formula in source] , now adjoin an oriented link basis [formula in source] and define This operator is implementable on matter Fock space tensored with the finite link space; it is fermion-even because each summand is a matter bilinear. Take the endpoint Gauss constraints to be [formula in source] and [formula in source] . T
Opening source excerpt. Formulas and the full argument remain in the original document.
Source location and explicit evidence links
tex-artefacts/toe_round7_parent_mirror.tex · lines 253 to 297
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