Actual slow moments of flat weighted mean fields #
The two-edge weight absorbs every fixed inverse-edge polynomial. Consequently
the actual derivatives of a supported mean field have global band bounds.
Finite torus averaging and radial integration preserve these bounds. All
derivatives in this file are iteratedFDeriv of the actual integral.
A global finite-prefix bound, with the discrete band and slow polynomial still visible. This is a proved consequence of the flat weighted class below.
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Flatness, rather than a new global-bound hypothesis, removes the radial edge loss. The input is the manuscript's concrete logarithmic mean class.
Exact higher chain rule for an affine map.
The unweighted slow strip keeps precisely the same band scales.
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A finite affine average; coordinate projections and torus insertion are special cases.
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Erase auxiliary X, bundling toFun, map_add, map_smul, cont.
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- NavierStokes.MeanMomentBounds.eraseAuxX = { toFun := fun (x : NavierStokes.PressureStream.Lift P) => (x.1, x.2.1, 0, x.2.2.2), map_add' := ⋯, map_smul' := ⋯, cont := ⋯ }
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Erase auxiliary Y, bundling toFun, map_add, map_smul, cont.
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- NavierStokes.MeanMomentBounds.eraseAuxY = { toFun := fun (x : NavierStokes.PressureStream.Lift P) => (x.1, x.2.1, x.2.2.1, 0), map_add' := ⋯, map_smul' := ⋯, cont := ⋯ }
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Aux X, given by (0, (0, (1, 0))).
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Aux Y, given by (0, (0, (0, 1))).
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Lifted torus average, given by PressureStream.torusAverage f (x.1, x.2.1).
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Lifted pressure mass, given by PressureStream.pressureMass f x.2.1.
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The actual pressure defect, lifted to the original strip, belongs to
S_α. There is no pressure-mass or differentiated-integral estimate premise.
Insert slow, bundling toFun, map_add, map_smul, cont.
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The same actual pressure moment as a function of only the slow variables.
The radial power is outside the auxiliary torus average, exactly as in the pressure and two integrated flux defects.
Every fixed radial moment of the actual torus mean is an unweighted slow coefficient of the same band order.