Manuscript X-G-ST@1 · X-G-ST.tex · section · 3c97567f

The completed scalar and three-tree interface

Frozen operators, switches, and the predecessor interface › The completed scalar and three-tree interface · lines 497–594

X-G-ST@1#eq:coordinates, X-G-ST@1#eq:tests, X-G-ST@1#eq:trees, X-G-ST@1#eq:PhiF

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We record the insertion target to make the counting unambiguous XC,STRecords,XFST. For , define , , , and by

In particular and .

The coordinate coefficients have zero position and velocity on and solve

Put

The affine decomposition is

With , the frozen three tree coefficients are

Here is the polarized quadratic coefficient of . These symbols mean the compact distributional kernels of the fixed-width tree sheet, not pointwise multiplication of singular fields.

The inherited expression is

The matter response equals . The scalar second-order pair in (eq:tests) and the three coefficients in (eq:trees) are retained once.

The inherited support distinctions remain: the scalar slot lies in ; the matter cubic has support in ; graviton slots of the other trees can reach . Full kernels are distributions. Suitable smooth scalar-slot contractions are elements of . No kernel-admission theorem is inferred from a scalar-test topology.

Displayed formulas in this passage

  • X-G-ST@1#eq:coordinates · line 516

  • X-G-ST@1#eq:tests · line 527

  • X-G-ST@1#eq:trees · line 553

  • X-G-ST@1#eq:PhiF · line 570

  • unlabeled · line 504

  • unlabeled · line 547

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