Complete controls for the scaled actual particular inverse #
The clock, normal, integration interval and native geometry are transported together. The forcing is the current target residual, with no source naturality assumption and no supplied modal-control record.
Modal inputs for the actual residual inverse #
The frame is the selected PhaseConstruction.frame. Its modal energy
estimate is derived from FrameData.energy_bound, including every nonzero
harmonic. The source is differentiated along the genuine shifted copy path;
geometric separation identifies its grouped Gaussian at every integration
time. All finite-jet constants precede the external label and lattice copy.
Actual frame jets, directly from the base and phase data of the selected construction. No regularity of a solved amplitude is an input.
The extra j² damping is dissipative. The same Gaussian rate and
error constant work for all nonzero harmonics, without a bound on j.
The same selected frame satisfies its actual slot kinematics.
A finite harmonic range introduces only a finite coefficient constant; the index type may already include every spatial label and band.
The source projection is built from its three actual frame columns.
The transverse copy coordinate is not a slow variable of the selected frame. The linear map also permits forgetting the auxiliary angle.
Equations
- NavierStokes.ActualParticularControl.nativeFrame d χ = NavierStokes.PrimaryCopyBridge.reindex d fun (q : P × ℝ) => χ q.1
Instances For
Frame argument as an element of ((P × Plane) × ℝ) →L[ℝ] (PhaseCalculus.Slow × ℝ).
Equations
- One or more equations did not get rendered due to their size.
Instances For
Frame domain, bundling scale, carrier, isOpen, one_le_scale.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The grouped Gaussian of this label, built from its actual copy geometry and its full padded integration rectangle.
Equations
- NavierStokes.ActualParticularControl.groupedEnvelope g r L W l n x = NavierStokes.WaveEnvelopeTransport.copyEnvelope (g l n) (r l n) (L l n) (W l n) x.2
Instances For
Uniform full jets of the actual shifted source. The source class is an input on the current residual, not on the solution or projected forcing. The Gaussian at an earlier integration time is derived by separation.
Joint coefficient, source-projection, and synthesis bounds of the literal copy frame. The full source path is used at every derivative order. No modal energy or projected forcing bound is supplied.
Instantiation of the input bound for the selected actual phase.
A fixed linear pullback preserves the order of all uniform quantifiers.
The actual three residual coefficients form one uniformly bounded source vector. No property of the inverse is assumed here.
Angle strip, given by CommonCoverClass.parameterStrip s (ContinuousLinearMap.fst ℝ P ℝ).
Equations
Instances For
Forget angle, given by ((ContinuousLinearMap.fst ℝ P ℝ).comp (ContinuousLinearMap.fst ℝ (P × ℝ) Plane)).prod (ContinuousLinearMap.snd ℝ (P × ℝ) Plane).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The additional angular variable is genuinely absent from the current source. Its introduction preserves the same moving strip weight.
A stage's finite harmonic range can be folded into the external label with one constant before both. This never infers uniformity over an unbounded harmonic family from separate class memberships.
Phase neighborhood, given by {x | x.1 ∈ s.domain ∧ χ x.1 ∈ D.carrier (l,n) ∧ ((g l n).coordinates k x.2).2 ∈ Ioo 0 (F.L (l,n))}.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Phase patch, given by phaseNeighborhood s F χ g l n k ∩ {x | ((g l n).coordinates k x.2).1 ∈ Icc (-(r l n)) (r l n)}.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The output majorant is this same native Gaussian on the phase patch; there is no replacement by an unweighted bound.
The reference/native control is assembled from the selected phase and the current source class. Its energy and all input jets are conclusions. Only the geometric separation and scale comparison remain geometric inputs.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The actual HR-source control, with an arbitrary fixed real projection.
The two applications part = realPart and part = imagPart are the two
literal Volterra solves in complexCopyCoefficients.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Transport argument, given by (φ.comp (ContinuousLinearMap.fst ℝ Q ℝ)).prod (rate • ContinuousLinearMap.snd ℝ Q ℝ).
Equations
- NavierStokes.ActualParticularControl.transportArgument φ rate = (φ ∘SL ContinuousLinearMap.fst ℝ Q ℝ).prod (rate • ContinuousLinearMap.snd ℝ Q ℝ)
Instances For
Indexed affine parameter/clock changes, with a single polynomial cost before every label. Translation centers have no derivative cost.
Transport all primitive frame fields with the same clock and normal
factors as ScaledTangentTransport.transportTangent.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Actual primitive jets after the same affine parameter and clock transport. The scalar bounds precede every index; the normal multiplier appears only in the two normal-scale fields.
Clock shortening exactly compensates the rescaling of the modal error rate. No lower bound on the clock rate is lost inside the exponential.
The transformed frame is precisely the tangent transport already used by the physical particular inverse, including its normal derivative.
The complete integration rectangle remains separated after the actual clock shortening and any covering refinement.
The literal selected frame after the zero-entry physical clock change.
Equations
- NavierStokes.ActualParticularControl.scaledSelectedFrame F φ rate normalScale i = NavierStokes.ActualParticularControl.transportedFrame (F.frame i) (⇑(φ i)) 0 (rate i) (normalScale i)
Instances For
All input jets at every target band are derived from the selected reference phase, bounded affine clock data, and the current residual source class on that target band. Neither transported modal energies nor transported output bounds are inputs.
Target domain, bundling scale, carrier, isOpen, one_le_scale.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Interval, given by (fun v => clock.value i.1 i.2*v) ⁻¹' F.V i.
Equations
Instances For
Length, given by F.L (l,n)/clock.value l n.
Equations
Instances For
Geometry, given by CopySolveCompatibility.transportGeometry (reference l n) (gap l n) 0 (clock.value l n) (clock.value_pos l n).ne'.
Equations
- NavierStokes.ScaledActualParticularControl.geometry reference gap clock l n = NavierStokes.CopySolveCompatibility.transportGeometry (reference l n) (gap l n) 0 (clock.value l n) ⋯
Instances For
Envelope, given by referenceP (F.lam (l,n)) (F.u (l,n)) (F.L (l,n)) (clock.value l n*v).
Equations
Instances For
Frame, given by scaledSelectedFrame F φ (fun i => clock.value i.1 i.2) (fun i => normal.value i.1 i.2) i.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Neighborhood, given by {x | x.1 ∈ s.domain ∧ φ (l,n) (χ x.1) ∈ D.carrier (l,n) ∧ ((g l n).coordinates k x.2).2 ∈ Ioo 0 (length F clock l n)}.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Patch, given by neighborhood s F χ φ clock g l n k ∩ {x | ((g l n).coordinates k x.2).1 ∈ Icc (-(r l n)) (r l n)}.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Every frame jet follows from the selected reference phase and the existing bounded affine/positive-scale data.
All fields of the scaled modal control are derived. The remaining quantitative inputs are affine/scale/rectangle facts about the chosen geometry and the current source coefficient class.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Overwrite only the source, exactly as realData and imagData do.
Equations
Instances For
Normal and clock transport commute with the selected slow-coordinate map. The transverse coordinate remains an auxiliary parameter.
The selected transported frame gives the exact angle-lifted STT tangent after inserting the current target source. No equality between the current source and a transported old source is used.
Transported tangent, constructed using ParticularWaveAssembly.angleTangent.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The full control for the literal target HR source and the exact
angle-lifted ScaledTangentTransport datum. Inserting the current source
does not require it to equal a scaled old source.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The clock change preserves the native Gaussian and polynomial geometry cost #
Geometry factor, given by 1 + coveringBound budget * (2+clock.upper+clock.lower⁻¹).
Equations
- NavierStokes.ScaledActualParticularControl.geometryFactor clock budget = 1 + NavierStokes.CommonCoverSolve.coveringBound budget * (2 + clock.upper + clock.lower⁻¹)
Instances For
Refining the cover and scaling its time column has polynomial cost. The constant uses only the already selected scale bounds and gap budget.
The actual active-window parameter and frequency scales #
Physical phi, given by ActualSignedGeometry.slowChange h (ChartScales.Q (chart i.2)) (ChartScales.Q (reference i.1 i.2)).
Equations
- One or more equations did not get rendered due to their size.
Instances For
Physical psi, given by PhysicalParticularWave.parameterChange h (ChartScales.Q (chart i.2)) (ChartScales.Q (reference i.1 i.2)).
Equations
- One or more equations did not get rendered due to their size.
Instances For
The same nonzero harmonic appears in both physical frequencies, so normal scaling is independent of its sign and size.
Slot reference, given by ActualSignedGeometry.slotGeometry sys hdet (slot l n) 0.
Equations
- NavierStokes.ScaledActualParticularControl.slotReference sys hdet slot l n = NavierStokes.ActualSignedGeometry.slotGeometry sys hdet (slot l n) 0
Instances For
Slot cost, given by 4*(geometryFactor clock budget)^2 * (25*CommonCoverClass.bandArgumentCost (TorusAverages.slotChart vr vt hdet) 0)^2.
Equations
- One or more equations did not get rendered due to their size.
Instances For
A full target control built from the original slot system, the selected reference phase, active-band bounds, and current HR coefficient classes. All clock, normal, affine and geometry bounds are supplied by the concrete active-window constructions; no energy or output-control premise remains.
Equations
- One or more equations did not get rendered due to their size.