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
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