Quadratic densities in the short-time rescaling #
These densities abbreviate the source field energy and its two fixed Gaussian weights in the short-time half-space argument.
noncomputable def
ESS.buShortQuadraticEnergy
(scale : ℝ)
(w : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(Dw : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3)
(z : CKN.Foundation.Parabolic.ParabolicPoint)
:
Quadratic velocity and spatial-gradient energy of the rescaled source field.
Equations
- One or more equations did not get rendered due to their size.
Instances For
noncomputable def
ESS.buShortTangentialDensity
(scale : ℝ)
(w : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(Dw : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3)
(z : CKN.Foundation.Parabolic.ParabolicPoint)
:
Tangential Gaussian density with the normal polynomial needed for the negative-phase error.
Equations
Instances For
noncomputable def
ESS.buShortWeightedPolynomialDensity
(scale a : ℝ)
(w : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(Dw : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3)
(z : CKN.Foundation.Parabolic.ParabolicPoint)
:
Fixed-parameter shifted Carleman density with the polynomial height factor needed for the shell estimates.
Equations
- ESS.buShortWeightedPolynomialDensity scale a w Dw z = ESS.buShortShiftedWeight scale a z * (1 + z.1 2) ^ 4 * ESS.buShortQuadraticEnergy scale w Dw z
Instances For
noncomputable def
ESS.buShortWeightedDensity
(scale a : ℝ)
(w : CKN.Foundation.Parabolic.ParabolicPoint → CKN.Foundation.Parabolic.Vec3)
(Dw : CKN.Foundation.Parabolic.ParabolicPoint → Fin 3 → CKN.Foundation.Parabolic.Vec3)
(z : CKN.Foundation.Parabolic.ParabolicPoint)
:
Fixed-parameter shifted Carleman quadratic density.
Equations
- ESS.buShortWeightedDensity scale a w Dw z = ESS.buShortShiftedWeight scale a z * ESS.buShortQuadraticEnergy scale w Dw z