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LeanPool.LiebThirring.Electrostatics.FaceMeasureGeometry

Geometry for the positive Voronoi face measure #

Half the separation of two nuclei, the height appearing in.

A frame chosen only to construct surface measure; its measure is independent of this choice, as established by bisectorSurfaceMeasure_eq.

noncomputable def LiebThirring.nuclearHalfDistance {M : ℕ} (R : Fin M → Position) (k l : Fin M) :

Half the separation of two nuclei, the height appearing in (6.1).

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    theorem LiebThirring.nuclearHalfDistance_pos {M : ℕ} (R : Fin M → Position) (hR : Function.Injective R) {k l : Fin M} (hkl : k ≠ l) :
    theorem LiebThirring.bisectorPlane_eq_affinePlane {M : ℕ} (R : Fin M → Position) (hR : Function.Injective R) {k l : Fin M} (hkl : k ≠ l) :
    theorem LiebThirring.planeHeight_bisector {M : ℕ} (R : Fin M → Position) (hR : Function.Injective R) {k l : Fin M} (hkl : k ≠ l) :
    planeHeight (bisectorNormal R k l) (midpoint ℝ (R k) (R l)) (R k) = nuclearHalfDistance R k l
    theorem LiebThirring.nuclearHalfDistance_le_norm_on_bisector {M : ℕ} (R : Fin M → Position) (hR : Function.Injective R) {k l : Fin M} (hkl : k ≠ l) {y : Position} (hy : y ∈ bisectorPlane R k l) :
    noncomputable def LiebThirring.bisectorSurfaceFrame {M : ℕ} (R : Fin M → Position) (hR : Function.Injective R) (k l : Fin M) (hkl : k ≠ l) :

    A frame chosen only to construct surface measure; its measure is independent of this choice, as established by bisectorSurfaceMeasure_eq.

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      noncomputable def LiebThirring.bisectorSurfaceMeasure {M : ℕ} (R : Fin M → Position) (hR : Function.Injective R) (k l : Fin M) (hkl : k ≠ l) :

      The usual Euclidean surface measure on a bisector plane.

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