OAI/MathematicalPhysics/Boltzmann/Compactness/UniformGain.lean
29 declarations, 0 contain sorry, 0 declared as axioms
Uniform elementary-sheet gain estimates
The incoming exponential tilt and the Gaussian in the companion velocity are kept separate. All regions below refer to the complete normalized kernel, including its singular velocity weight.
- def
OAI.BoltzmannNonuniqueness.UniformGain.exponentialTiltline 26 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.measurable_exponentialTiltline 28 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.measurable_weightRatioline 32 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.ratio_boundline 35 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.normalized_restriction_leline 54Source documentation
The weight transfer can be applied on any measurable portion of the chart.
theorem normalized_restriction_le (c : Measure Velocity) (q : ℝ) (v : Velocity) {S T : Set Coordinates} (hS : MeasurableSet S) (hT : MeasurableSet T) (hST : S ⊆ T) {B : ℝ} (hB : 0 ≤ B) (hb : ∀ y ∈ S, Real.exp (-‖companionVelocity y.1 (chart v y.1 y.2.1 y.2.2) v‖ ^ 2) ≤ B) : normalizedMeasure c q v S ≤ ENNReal.ofReal (tiltConstant * B) * ChartKernel.measure (c.withDensity exponentialTilt) (weightRatio q v) v T := by …Mentions: OAI.BoltzmannNonuniqueness.Velocity, OAI.BoltzmannNonuniqueness.companionVelocity, OAI.BoltzmannNonuniqueness.ChartKernel.measure, OAI.BoltzmannNonuniqueness.UniformGain.exponentialTilt
- theorem
OAI.BoltzmannNonuniqueness.UniformGain.measurableSet_ballRegionline 81 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.weight_ball_measure_boundline 84 - def
OAI.BoltzmannNonuniqueness.UniformGain.ballBoundline 92 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.tilted_ball_boundline 95 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.tilted_tail_ball_boundline 107 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.normalized_ball_boundline 126 - def
OAI.BoltzmannNonuniqueness.UniformGain.radiusline 139 - def
OAI.BoltzmannNonuniqueness.UniformGain.shellline 142 - def
OAI.BoltzmannNonuniqueness.UniformGain.incomingTailline 145 - def
OAI.BoltzmannNonuniqueness.UniformGain.companionTailline 147 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.measurable_radiusline 150 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.measurableSet_shellline 153 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.measurableSet_incomingTailline 157 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.measurableSet_companionTailline 160 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.shell_subset_ballline 166 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.shell_subset_unionline 171 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.normalized_cold_shell_boundline 180 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.normalized_hot_shell_boundline 201 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.normalized_shell_bound_rawline 217 - def
OAI.BoltzmannNonuniqueness.UniformGain.shellConstantline 234 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.geometricTotalConstant_nonnegline 237 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.shellConstant_nonnegline 242 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.shell_coefficient_boundline 248 - theorem
OAI.BoltzmannNonuniqueness.UniformGain.normalized_shell_boundline 282Source documentation
The full normalized kernel has a uniform Gaussian bound on every shell.
theorem normalized_shell_bound {q d R L : ℝ} (hq₁ : 1 < q) (hq₂ : q < 2) (hd : 0 ≤ d) (hdmax : d ≤ 1 / 8) (hR : 1 ≤ R) {v : Velocity} (hv : transverse v ≠ 0) {ρ : Measure ℝ} [IsProbabilityMeasure ρ] (hρ : AxialMoment ρ L) : normalizedMeasure (sheetLaw d ρ) q v (shell v R) ≤ ENNReal.ofReal (shellConstant q L * R ^ 2 * Real.exp (-(3 / 32) * R ^ 2)) := …Mentions: OAI.BoltzmannNonuniqueness.Velocity, OAI.BoltzmannNonuniqueness.UniformGain.shell, OAI.BoltzmannNonuniqueness.UniformGain.shellConstant