Manuscript XVI-B@1 · XVI-B.tex · section · 6a0abffd

Prepared-source input

Setting, notation, and explicit inputs › Prepared-source input · lines 386–438

XVI-B@1#eq:actualsource, XVI-B@1#eq:time-layer, XVI-B@1#eq:trace-input, XVI-B@1#eq:polarization

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The supplied XII-C source theorem gives the Euler source of the selected weighted cubic density as

For a time-only switch, its reported general layer formula is

The coefficient labels and belong to XII-C. Their general component formulas are not reconstructed here XIIC.

For the calculations below, the necessary explicit input is the reported pure-trace restriction:

In that sector, XII-C reports , so the coefficient of in (eq:time-layer) vanishes.

These are imported formulas, not a new derivation of the full cubic Euler source. For fixed smooth input fields, the source evaluations considered below are smooth tensor fields.

The quadratic polarization convention is

for each homogeneous quadratic map . Complex inputs are evaluated through complex bilinear extension, not through a Hermitian polarization.

Displayed formulas in this passage

  • XVI-B@1#eq:actualsource · line 390

  • XVI-B@1#eq:time-layer · line 396

  • XVI-B@1#eq:trace-input · line 408

  • XVI-B@1#eq:polarization · line 428