Manuscript X-A-conv-ST@1 · X-A-conv-ST.tex · section · 8ca47088

Fields, formal order, and gauge algebra

The fully specified convolution contract › Fields, formal order, and gauge algebra · lines 344–412

X-A-conv-ST@1#eq:metricjet, X-A-conv-ST@1#eq:switch, X-A-conv-ST@1#eq:gaugealgebra, X-A-conv-ST@1#eq:gaugetransformation

Back to manuscript

The smooth off-shell inputs are

No decay, equation-of-motion quotient, gravitational constraint, or gauge-fixed quotient is imposed. The scalar is massless.

The formal metric jet is

There is no factor in the definition of . Statements modulo mean coefficient identities, not convergence of a numerical perturbation series.

Set and , where the Euclidean norm is used only for supports and convolution. Define

Freeze

Then on , and .

For a vector field , write

The algebra fixed before the calculation is

Indices are raised and lowered with . The switch is fixed background data.

For ,

gives

The scalar transforms by the same formal pullback.

Displayed formulas in this passage

  • X-A-conv-ST@1#eq:metricjet · line 357

  • X-A-conv-ST@1#eq:switch · line 378

  • X-A-conv-ST@1#eq:gaugealgebra · line 393

  • X-A-conv-ST@1#eq:gaugetransformation · line 406

  • unlabeled · line 347

  • unlabeled · line 368

  • unlabeled · line 387

  • unlabeled · line 401