Coherence of the constructed primary waves #
The phase, coefficient, cutoff, and chart in this file are the actual
CorrectionInitialization.ActualPrimary constructors. Their differentiated
curl correction and Gaussian term are transported on the whole free lift.
An invertible chart transports the actual derivative, including at points where Lean's derivative is defined to be zero.
The literal absolute chart and its directions #
Chart point: an abbreviation for LocalSignedRequest.Point × ℝ.
Equations
Instances For
Absolute: an abbreviation for AbsolutePoint × ℝ.
Equations
Instances For
Absolute chart, bundling toFun, invFun, left_inv, right_inv and the required
compatibility proofs.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Absolute radius, given by x.1.1.1.
Equations
Instances For
Absolute radial, given by (((1,(0,0)), RadialPullback.radialJacobian (ChartScales.radialExponent h) x.1.1.1 • radialVector), 0).
Equations
- One or more equations did not get rendered due to their size.
Instances For
Absolute angular, given by (0,1).
Equations
Instances For
Absolute fast, given by (((0,(0,0)),temporalVector),0).
Equations
Instances For
The actual cut coefficient, corrected wave, and Gaussian field #
Absolute cut amplitude, given by periodicGaussian j L x.1.2 • absoluteAmplitude j L x.1.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Absolute exact amplitude, constructed using CurlClassBounds.realizedCoefficient.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Absolute velocity, defined pointwise by (vectorMode 1 (absolutePhase j L) (absoluteExactAmplitude j L) x i).re.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Absolute gaussian coefficient, given by along absoluteFast (fun y => periodicGaussian j L y.1.2) x • absoluteAmplitude j L x.1.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Absolute gaussian, defined pointwise by (vectorMode 1 (absolutePhase j L) (absoluteGaussianCoefficient j L) x i).re.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Full-fiber transport of the coefficient actually used by the iteration. No equality of corrected fields, nor a tangency assertion, is an input.
Exact comparison of two genuine common-cover bands #
Ordinary regularity before restricting to a bounded strip #
Positive chart, given by {x | 0 < x.1.2.1.1}.
Equations
Instances For
Positive radial chart, given by {x | 0 < x.1.1 ∧ 0 < x.1.2.1.1}.
Equations
- NavierStokes.ActualPrimaryCoherence.positiveRadialChart = {x : NavierStokes.ActualPrimaryCoherence.ChartPoint | 0 < x.1.1 ∧ 0 < x.1.2.1.1}
Instances For
Positive absolute, given by {x | 0 < x.1.1.2.2}.
Equations
Instances For
Positive radial absolute, given by {x | 0 < x.1.1.1 ∧ 0 < x.1.1.2.2}.
Equations
- NavierStokes.ActualPrimaryCoherence.positiveRadialAbsolute = {x : NavierStokes.ActualPrimaryCoherence.Absolute | 0 < x.1.1.1 ∧ 0 < x.1.1.2.2}
Instances For
Absolute normal, given by phaseNormal absoluteRadius absoluteRadial absoluteAngular absoluteAxial (absolutePhase j L).
Equations
- One or more equations did not get rendered due to their size.
Instances For
Amplitude radius, given by PrimaryTargetBounds.profileRadius h (nativeSlow L x.1).
Equations
- One or more equations did not get rendered due to their size.
Instances For
Periodicity on the genuine common covers #
Chart deck, given by ((0, ((0,0), TorusAverages.latticePoint k)),0).
Equations
Instances For
Tangency of the actual native pulse #
Chart radius linear, given by (ContinuousLinearMap.fst ℝ ℝ _).comp (ContinuousLinearMap.fst ℝ _ ℝ).
Equations
- One or more equations did not get rendered due to their size.
Instances For
Chart radial curve, constructed using PhysicalResidualTZ.swapCylinder.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Tangency holds on every band. A valid native cover proves it first, then the exact absolute normal and amplitude laws remove any index restriction.
Literal real corrected field, with the radial connection term included.
The absolute free lift evaluated on the actual physical cylindrical graph.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Physical phase, defined pointwise by absolutePhase j L (physicalLift z).
Equations
Instances For
Physical amplitude, defined pointwise by absoluteCutAmplitude j L (physicalLift z).
Equations
Instances For
Lifted phase, defined pointwise by (chartCoefficients j L).phase n (PhysicalResidualTZ.swapCylinder x).
Equations
Instances For
Lifted amplitude, defined pointwise by ((chartCoefficients j L).withCutoff (chartCutoff j L)).amplitude n (PhysicalResidualTZ.swapCylinder x).
Equations
- One or more equations did not get rendered due to their size.
Instances For
Lifted domain, given by PhysicalResidualTZ.swapCylinder ⁻¹' positiveRadialChart.
Equations
Instances For
Physical angular, given by (0,ProblemStatement.coordinateVector 1).
Equations
Instances For
Physical potential, given by PhysicalCurlCovariance.referencePotential 1 (physicalPhase j L) (physicalAmplitude j L).
Equations
- One or more equations did not get rendered due to their size.
Instances For
One fixed radius for each original label, chosen from its actual physical scale and the positive inner support radius.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The complete periodic potential gives a forward representation at every positive cylindrical radius, including angles outside the chosen inverse chart.
One actual Cartesian potential for every primary label #
No band index occurs in this Cartesian potential. The cutoff is the original periodic Gaussian, and the polar chart is chosen from its full-turn-compatible values.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Cartesian velocity, given by SpatialCurl.spatialCurl (cartesianPotential j L).
Equations
Instances For
Every actual band velocity is the rotating-frame representation of the curl of the same constructed Cartesian potential. This includes all positive radii and all angles, without a native-cover restriction.
Physical pressure, defined pointwise by absolutePressureMode j L (physicalLift z).