OAI/MathematicalPhysics/NavierStokes/ForcedComputation/Scalar/PlaneHeatTimeContinuity.lean

GitHub source file

19 declarations, 0 contain sorry, 0 declared as axioms

Operator-norm continuity of Gaussian heat operators at every strictly positive time.

  1. def OAI.ForcedComputation.PlaneHeat.timeCore line 14
  2. def OAI.ForcedComputation.PlaneHeat.timeCoefficient line 15
  3. def OAI.ForcedComputation.PlaneHeat.timeEnvelope line 16
  4. def OAI.ForcedComputation.PlaneHeat.timeDerivativeEnvelope line 18
  5. theorem OAI.ForcedComputation.PlaneHeat.oneDim_time_le line 21
  6. theorem OAI.ForcedComputation.PlaneHeat.kernel_time_le line 38
  7. theorem OAI.ForcedComputation.PlaneHeat.derivative_time_le line 48
  8. theorem OAI.ForcedComputation.PlaneHeat.timeCore_integrable line 57
  9. theorem OAI.ForcedComputation.PlaneHeat.timeMoment_integrable line 60
  10. theorem OAI.ForcedComputation.PlaneHeat.product_integrable line 65
  11. theorem OAI.ForcedComputation.PlaneHeat.timeEnvelope_integrable line 69
  12. theorem OAI.ForcedComputation.PlaneHeat.timeDerivativeEnvelope_integrable line 74
  13. theorem OAI.ForcedComputation.PlaneHeat.oneDim_time_continuousAt line 92
  14. theorem OAI.ForcedComputation.PlaneHeat.kernel_time_continuousAt line 97
  15. theorem OAI.ForcedComputation.PlaneHeat.derivative_time_continuousAt line 101
  16. theorem OAI.ForcedComputation.PlaneHeat.kernel_l1_tendsto line 111

    Source documentation

    Gaussian kernels are continuous in L1 at every strictly positive time.

    theorem kernel_l1_tendsto {t : ℝ} (ht : 0 < t) :
        Tendsto (fun s => ∫ y, |kernel s y - kernel t y|) (𝓝 t) (𝓝 0) := by
    …

    Mentions: OAI.ForcedComputation.PlaneHeat.kernel

  17. theorem OAI.ForcedComputation.PlaneHeat.kernelDerivative_l1_tendsto line 141

    Source documentation

    The Cartesian Gaussian derivatives are also continuous in L1 at positive time.

    theorem kernelDerivative_l1_tendsto {t : ℝ} (ht : 0 < t) (j : Fin 2) :
        Tendsto (fun s => ∫ y, |kernelDerivative s j y - kernelDerivative t j y|) (𝓝 t) (𝓝 0) := by
    …

    Mentions: OAI.ForcedComputation.PlaneHeat.kernelDerivative

  18. theorem OAI.ForcedComputation.PlaneHeat.continuous_heatOperator line 173

    Source documentation

    Heat operators depend continuously on positive time in the operator norm on C_b^k.

    theorem continuous_heatOperator (k : ℕ) :
        Continuous (fun t : {t : ℝ // 0 < t} => heatOperator F k t.val t.property) := by
    …

    Mentions: OAI.ForcedComputation.PlaneHeat.heatOperator

  19. theorem OAI.ForcedComputation.PlaneHeat.continuous_gradientOperator line 183

    Source documentation

    The singular gradient bound causes no loss of operator continuity away from time zero.

    theorem continuous_gradientOperator (k : ℕ) (j : Fin 2) :
        Continuous (fun t : {t : ℝ // 0 < t} => gradientOperator F k t.val t.property j) := by
    …

    Mentions: OAI.ForcedComputation.PlaneHeat.gradientOperator