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Centroid mass and the distance-annulus radius

Definition
Esgk_ThinAnnulus

by mysticflounder · Oct 20, 2026 · Mathlib 0df444a (Lean v4.33.1)

discrete-geometrydistinct-distances

For an indexed configuration p=(p1,…,pn)p=(p_1,\dots,p_n)p=(p1​,…,pn​) of points in the plane with centroid c(p)c(p)c(p) (configCentroid p) and distance values R(p)={∣pi−pj∣:i≠j}R(p)=\{|p_i-p_j|: i\ne j\}R(p)={∣pi​−pj​∣:i=j}, this module defines three real numbers.

  1. centroidSquaredMass p: M(p)=∑i∣pi−c(p)∣2M(p)=\sum_{i}|p_i-c(p)|^2M(p)=∑i​∣pi​−c(p)∣2.
  2. distanceAnnulusRadiusSq p:
ρ2(p)=1n(3∑r∈R(p)r2−M(p)).\rho^2(p)=\frac1n\Bigl(3\sum_{r\in R(p)}r^2-M(p)\Bigr).ρ2(p)=n1​(3r∈R(p)∑​r2−M(p)).
  1. distanceAnnulusRadius p: the real square root ρ(p)=ρ2(p)\rho(p)=\sqrt{\rho^2(p)}ρ(p)=ρ2(p)​.

For an injective configuration with n≥1n\ge1n≥1 and no four points on a common circle, every ∣pi−c(p)∣2|p_i-c(p)|^2∣pi​−c(p)∣2 is at most ρ2(p)\rho^2(p)ρ2(p), and the theorem Esgk.thin_annulus_sq_of_noFourCocircular bounds it from below in terms of the number of distinct distances.

Formalization Note The quantity ρ2(p)\rho^2(p)ρ2(p) is a formula, not a square, and distanceAnnulusRadius applies Real.sqrt, which returns 000 for negative arguments. For n=0n=0n=0 the division by nnn gives 000 in Lean.

Definition code
/-
Copyright (c) 2026 Adam McKenna. All rights reserved.
Released under Apache 2.0 license as described in the file LICENSE.
Authors: Adam McKenna
-/

import Definitions.Def_Esgk_Energy
import Definitions.Def_Esgk_Foundation
import Definitions.Def_Esgk_ConfigurationCentroid

namespace Esgk

open EuclideanGeometry
open scoped BigOperators
variable {n : ℕ}

noncomputable def centroidSquaredMass (p : Config n) : ℝ :=
  ∑ i, dist (p i) (configCentroid p) ^ 2

noncomputable def distanceAnnulusRadiusSq (p : Config n) : ℝ :=
  (3 * (∑ r ∈ OrderedDistanceValues p, r ^ 2) - centroidSquaredMass p) / (n : ℝ)

noncomputable def distanceAnnulusRadius (p : Config n) : ℝ :=
  Real.sqrt (distanceAnnulusRadiusSq p)

end Esgk

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