OAI/MathematicalPhysics/Boltzmann/Collision/SheetIntervals.lean
39 declarations, 0 contain sorry, 0 declared as axioms
Summing the normalized sheet kernel
The Gaussian shell estimate yields a finite constant independent of the transverse width, the axial law, and the output velocity off the axis.
- def
OAI.BoltzmannNonuniqueness.SheetTotal.shellTermline 27 - theorem
OAI.BoltzmannNonuniqueness.SheetTotal.shellTerm_nonnegline 30 - theorem
OAI.BoltzmannNonuniqueness.SheetTotal.summable_shellTermline 34 - def
OAI.BoltzmannNonuniqueness.SheetTotal.boundline 51 - theorem
OAI.BoltzmannNonuniqueness.SheetTotal.bound_lt_topline 55 - theorem
OAI.BoltzmannNonuniqueness.SheetTotal.cover_by_shellsline 63 - theorem
OAI.BoltzmannNonuniqueness.SheetTotal.normalized_total_boundline 79Source documentation
Uniform finiteness and the complete gain bound for an elementary sheet.
theorem normalized_total_bound {q d L : ℝ} (hq₁ : 1 < q) (hq₂ : q < 2) (hd : 0 ≤ d) (hdmax : d ≤ 1 / 8) {v : Velocity} (hv : transverse v ≠ 0) {ρ : Measure ℝ} [IsProbabilityMeasure ρ] (hρ : AxialMoment ρ L) : normalizedChartGain (sheetLaw d ρ) q v ≤ bound q L := by …Mentions: OAI.BoltzmannNonuniqueness.Velocity, OAI.BoltzmannNonuniqueness.normalizedChartGain, OAI.BoltzmannNonuniqueness.SheetTotal.bound
- theorem
OAI.BoltzmannNonuniqueness.SheetTotal.normalized_total_lt_topline 99 - def
OAI.BoltzmannNonuniqueness.SheetClass.fiberline 131 - theorem
OAI.BoltzmannNonuniqueness.SheetClass.measurable_fiberline 134 - theorem
OAI.BoltzmannNonuniqueness.SheetClass.gain_eq_lintegral_fiberline 137 - theorem
OAI.BoltzmannNonuniqueness.SheetClass.gain_bindline 144 - def
OAI.BoltzmannNonuniqueness.SheetClass.IsElementaryline 153Source documentation
The elementary class allows both zero transverse width and arbitrary axial atoms.
def IsElementary (L : ℝ) (c : Measure Velocity) : Prop := …
Mentions: OAI.BoltzmannNonuniqueness.Velocity
- theorem
OAI.BoltzmannNonuniqueness.SheetClass.elementary_boundline 157 - theorem
OAI.BoltzmannNonuniqueness.SheetClass.mixture_boundline 164 - theorem
OAI.BoltzmannNonuniqueness.SheetClass.domination_boundline 178 - theorem
OAI.BoltzmannNonuniqueness.SheetApplication.gain_const_mul_rightline 214 - theorem
OAI.BoltzmannNonuniqueness.SheetApplication.gain_H_eqline 230 - theorem
OAI.BoltzmannNonuniqueness.SheetApplication.ae_transverse_ne_zeroline 242 - theorem
OAI.BoltzmannNonuniqueness.SheetApplication.nonnegativeGain_sheet_boundline 257Source documentation
The original nonnegative hard-sphere gain obeys the sheet domination bound, conditionally only on the published Carleman identity.
theorem nonnegativeGain_sheet_bound (hcarleman : Published.GPV2009CarlemanInput) {ι : Type*} [MeasurableSpace ι] {ν : Measure ι} [IsProbabilityMeasure ν] {M : ι → Measure Velocity} (hM : Measurable M) {q L : ℝ} (hq₁ : 1 < q) (hq₂ : q < 2) (hc : ∀ᵐ i ∂ν, IsElementary L (M i)) {f : Velocity → ℝ≥0∞} (hf : Measurable f) {A : ℝ≥0∞} (hdom : volume.withDensity f ≤ A • ν.bind M) : ∀ᵐ v : Velocity ∂volume, nonnegativeGain f (fun ξ => ENNReal.ofReal (H q ξ)) v ≤ ENNReal.ofReal (H q v) * (A * SheetTotal.bound q L) := by …Mentions: OAI.BoltzmannNonuniqueness.Published.GPV2009CarlemanInput, OAI.BoltzmannNonuniqueness.Velocity, OAI.BoltzmannNonuniqueness.nonnegativeGain, OAI.BoltzmannNonuniqueness.SheetTotal.bound
- def
OAI.BoltzmannNonuniqueness.SheetTightness.tailRegionline 300 - def
OAI.BoltzmannNonuniqueness.SheetTightness.tailBoundline 303 - theorem
OAI.BoltzmannNonuniqueness.SheetTightness.tendsto_tailBoundline 306 - theorem
OAI.BoltzmannNonuniqueness.SheetTightness.measurableSet_tailRegionline 310 - theorem
OAI.BoltzmannNonuniqueness.SheetTightness.cover_tailline 314 - theorem
OAI.BoltzmannNonuniqueness.SheetTightness.normalized_tail_boundline 332 - theorem
OAI.BoltzmannNonuniqueness.SheetTightness.uniform_tailline 345Source documentation
A single truncation works for every width, axial law and off-axis output.
theorem uniform_tail {q L : ℝ} (hq₁ : 1 < q) (hq₂ : q < 2) {ε : ℝ≥0∞} (hε : 0 < ε) : ∃ N : ℕ, ∀ n ≥ N, ∀ (d : ℝ) (ρ : Measure ℝ) (_ : IsProbabilityMeasure ρ) (_ : 0 ≤ d) (_ : d ≤ 1 / 8) (_ : AxialMoment ρ L) (v : Velocity) (_ : transverse v ≠ 0), normalizedMeasure (sheetLaw d ρ) q v (tailRegion v n) ≤ ε := by …Mentions: OAI.BoltzmannNonuniqueness.Velocity, OAI.BoltzmannNonuniqueness.SheetTightness.tailRegion
- def
OAI.BoltzmannNonuniqueness.SheetIntervals.intervalRegionline 387 - theorem
OAI.BoltzmannNonuniqueness.SheetIntervals.mem_intervalRegionline 390 - theorem
OAI.BoltzmannNonuniqueness.SheetIntervals.measurableSet_intervalRegionline 398 - def
OAI.BoltzmannNonuniqueness.SheetIntervals.intervalFiberline 403 - theorem
OAI.BoltzmannNonuniqueness.SheetIntervals.intervalFiber_le_sliceline 409 - theorem
OAI.BoltzmannNonuniqueness.SheetIntervals.interval_gain_eqline 456 - def
OAI.BoltzmannNonuniqueness.SheetIntervals.intervalBoundline 480 - theorem
OAI.BoltzmannNonuniqueness.SheetIntervals.weight_interval_boundline 483 - theorem
OAI.BoltzmannNonuniqueness.SheetIntervals.weight_interval_measure_boundline 505 - theorem
OAI.BoltzmannNonuniqueness.SheetIntervals.normalized_interval_boundline 514Source documentation
The axial interval bound includes the complete ratio
H(ξ)/H(v).theorem normalized_interval_bound {q d R L a b : ℝ} (hq₁ : 1 < q) (hq₂ : q < 2) (hd : 0 ≤ d) (hdmax : d ≤ 1 / 8) (hR : 0 < R) (hab : a < b) {v : Velocity} (hv : transverse v ≠ 0) {ρ : Measure ℝ} [IsProbabilityMeasure ρ] (hρ : AxialMoment ρ L) : normalizedMeasure (sheetLaw d ρ) q v (intervalRegion v R a b) ≤ ENNReal.ofReal tiltConstant * ENNReal.ofReal (4 * L) * intervalBound q R (b - a) := by …Mentions: OAI.BoltzmannNonuniqueness.Velocity, OAI.BoltzmannNonuniqueness.SheetIntervals.intervalRegion, OAI.BoltzmannNonuniqueness.SheetIntervals.intervalBound
- theorem
OAI.BoltzmannNonuniqueness.SheetIntervals.intervalBound_monoline 532 - theorem
OAI.BoltzmannNonuniqueness.SheetIntervals.intervalBound_tendsto_zeroline 543