OAI/Geometry/EinsteinFour/QuarticEnergy.lean
6 declarations, 0 contain sorry, 0 declared as axioms
The full scalar quartic estimate, with both energy and spectral defects.
- def
OAI.PositiveEinsteinFour.QuarticEnergy.projectionCoefficientline 15Source documentation
The coefficient
gin the weighted Hessian projection bound.def projectionCoefficient (v y σ ρ : ℝ) : ℝ := …
- theorem
OAI.PositiveEinsteinFour.QuarticEnergy.projectionCoefficient_leline 19Source documentation
The normalized spectral parameter controls the actual projection cost.
theorem projectionCoefficient_le {v b r σ ρ W : ℝ} (hv : 0 ≤ v) (hr : 1 ≤ r) (hr2 : r ≤ 2) (hvr : v * r ≤ 2) (hσ : σ = (3 * r - r ^ 3) / 2) (hρ : ρ ^ 2 = 1 - σ ^ 2) : projectionCoefficient v (b + W) σ ρ ≤ projectionBound v b (v * r - v) W := by …Mentions: OAI.PositiveEinsteinFour.QuarticEnergy.projectionCoefficient
- theorem
OAI.PositiveEinsteinFour.QuarticEnergy.energy_zero_defect_identityline 30Source documentation
At zero energy defects the expression in (19) is exactly the scalar form bounded by the homogeneous inequality (20).
theorem energy_zero_defect_identity (v b V W H Hb P Q : ℝ) (hP : 0 ≤ P) (hQ : 0 ≤ Q) : quarticEnergy v b (P ^ 2) (Q ^ 2) (projectionBound v b V W) (projectionBound b v W V) H Hb (P ^ 2) (Q ^ 2) = (3 / 10) * (P + Q) * ((1 - 3 * (v - b) / 8) * P ^ 3 + (1 - 3 * (b - v) / 8) * Q ^ 3) + (27 / 320) * (P + Q) ^ 2 * (projectionBound v b V W * P ^ 2 + projectionBound b v W V * Q ^ 2) - (2 / 5) * (17 / 10) * (P ^ 2 + Q ^ 2) * (P ^ 2 / v + Q ^ 2 / b) := by … - theorem
OAI.PositiveEinsteinFour.QuarticEnergy.energy_zero_defect_mono_coefficientsline 48Source documentation
Increasing the fixed radial coefficients increases the zero-defect energy expression. The remaining coefficients are irrelevant at zero defect.
theorem energy_zero_defect_mono_coefficients (v b H Hb P Q g gb g' gb' : ℝ) (hg : g ≤ g') (hgb : gb ≤ gb') : quarticEnergy v b (P ^ 2) (Q ^ 2) g gb H Hb (P ^ 2) (Q ^ 2) ≤ quarticEnergy v b (P ^ 2) (Q ^ 2) g' gb' H Hb (P ^ 2) (Q ^ 2) := by … - theorem
OAI.PositiveEinsteinFour.QuarticEnergy.quartic_energy_boundline 64Source documentation
The entire right side of equation (19) is bounded by the negative quartic term, retaining the actual spectral coefficients and arbitrary nonnegative energy defects. The normalized eigenvalue parameters supply the spectral restrictions rather than assuming axial curvature.
theorem quartic_energy_bound {v b r s σ τ ρ χ P Q e f : ℝ} (hv : 0 < v) (hb : 0 < b) (hr : 1 ≤ r) (hr2 : r ≤ 2) (hs : 1 ≤ s) (hs2 : s ≤ 2) (hspectral : v * r + b * s ≤ 2) (hσ : σ = (3 * r - r ^ 3) / 2) (hρ : ρ ^ 2 = 1 - σ ^ 2) (hτ : τ = (3 * s - s ^ 3) / 2) (hχ : χ ^ 2 = 1 - τ ^ 2) (hP : 0 ≤ P) (hQ : 0 ≤ Q) (he : P ^ 2 ≤ e) (hf : Q ^ 2 ≤ f) : quarticEnergy v b (P ^ 2) (Q ^ 2) (projectionCoefficient v (b * s) σ ρ) (projectionCoefficient b (v * r) τ χ) (defectCoefficient v (b * s)) (defectCoefficient b (v * r)) e f ≤ -(2 / 5 - 3 * v * b / 10) * (9 / 25) * …Mentions: OAI.PositiveEinsteinFour.QuarticEnergy.projectionCoefficient
- theorem
OAI.PositiveEinsteinFour.QuarticEnergy.quartic_energy_bound_gradientline 104Source documentation
The same estimate in the squared gradient variables of the combined integrand:
a = |p|²andd = |q|².theorem quartic_energy_bound_gradient {v b r s σ τ ρ χ a d e f : ℝ} (hv : 0 < v) (hb : 0 < b) (hr : 1 ≤ r) (hr2 : r ≤ 2) (hs : 1 ≤ s) (hs2 : s ≤ 2) (hspectral : v * r + b * s ≤ 2) (hσ : σ = (3 * r - r ^ 3) / 2) (hρ : ρ ^ 2 = 1 - σ ^ 2) (hτ : τ = (3 * s - s ^ 3) / 2) (hχ : χ ^ 2 = 1 - τ ^ 2) (ha : 0 ≤ a) (hd : 0 ≤ d) (he : (5 / 3) * a ≤ e) (hf : (5 / 3) * d ≤ f) : quarticEnergy v b ((5 / 3) * a) ((5 / 3) * d) (projectionCoefficient v (b * s) σ ρ) (projectionCoefficient b (v * r) τ χ) (defectCoefficient v (b * s)) (defectCoefficient b (v * r)) e f ≤ -(2 / 5 - 3 * v * b / 10) * (a + d) * (a / v + d / b) := by …Mentions: OAI.PositiveEinsteinFour.QuarticEnergy.projectionCoefficient