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LeanPool.LiebThirring.Electrostatics.ScreenedRegularityBasic

Finiteness and continuity of the screened potential #

The extended screened potential and its real representative agree on their finite locus.

noncomputable def LiebThirring.screenedPotentialReal {M : ℕ} (Z : NNReal) (R : Fin M → Position) (x : Position) :

The real form of the shared extended screened potential.

Equations
Instances For
    theorem LiebThirring.nuclear_separation_le_twice_dist {M : ℕ} (R : Fin M → Position) (k p : Fin M) {x : Position} (hx : x ∈ closedVoronoiCell R k) :
    ‖R p - R k‖ ≤ 2 * ‖x - R p‖

    Every retained pole is separated from a closed nearest-nucleus cell.

    theorem LiebThirring.ne_nucleus_of_mem_closedVoronoiCell {M : ℕ} (R : Fin M → Position) (hR : Function.Injective R) (k p : Fin M) (hpk : p ≠ k) {x : Position} (hx : x ∈ closedVoronoiCell R k) :
    x ≠ R p
    theorem LiebThirring.screenedPotential_eq_on_closedVoronoiCell {M : ℕ} (Z : NNReal) (R : Fin M → Position) (k : Fin M) {x : Position} (hx : x ∈ closedVoronoiCell R k) :
    screenedPotential Z R x = ∑ p ∈ Finset.univ.erase k, ↑Z * coulombKernel x (R p)

    The shared minimum is the explicit formula on every closed cell.

    theorem LiebThirring.screenedPotential_ne_top {M : ℕ} (hM : 1 ≤ M) (Z : NNReal) (R : Fin M → Position) (hR : Function.Injective R) (x : Position) :

    Distinct nuclei make the screened potential finite even at a nucleus.

    Extended continuity also holds without separation of the nuclei.

    The real closed-cell formula has no singular retained denominators.