The inverse-square field and its divergence #
The gradient of the inverse-square potential, with its scalar factor written by squared norm.
The inverse-square potential has precisely the displayed gradient field.
Coordinate trace of the derivative on physical Euclidean space.
Equations
- LiebThirring.positionDivergence V x = ∑ i : Fin 3, ((fderiv ℝ V x) ((EuclideanSpace.basisFun (Fin 3) ℝ) i)).ofLp i
Instances For
Exact divergence of the inverse-square gradient off the nucleus.
Applying the derivative of the scaled cutoff in the radial direction.
theorem
LiebThirring.positionDivergence_smul
(f : Position → ℝ)
(V : Position → Position)
(x : Position)
(hf : DifferentiableAt ℝ f x)
(hV : DifferentiableAt ℝ V x)
:
positionDivergence (fun (y : Position) => f y • V y) x = f x * positionDivergence V x + (fderiv ℝ f x) (V x)
Divergence product rule for a scalar and a vector field at a differentiability point.
theorem
LiebThirring.positionDivergence_cutoff_field
(c x : Position)
(T : ℝ)
(hx : x ≠ c)
:
positionDivergence (fun (y : Position) => exteriorFluxCutoff c T y • exteriorInverseSquareField c y) x = exteriorFluxCutoff c T x * (2 / ‖x - c‖ ^ 4) - exteriorFluxDefect (T⁻¹ • (x - c)) * (2 / ‖x - c‖ ^ 4)
The exact pointwise cutoff divergence, including its gradient error.