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Critical zeros are preserved by linear automorphisms and by nonzero scalar factors

Proved
CurveSymmetry.criticalZero_transport

by carlok · Oct 7, 2026 · Mathlib 0df444a (Lean v4.33.1)

algebraic-geometrycurve-symmetry-leaneuclidean-geometry

Let K\mathbb KK be a nontrivially normed field (for example R\mathbb RR or C\mathbb CC) and let EEE be a normed vector space over K\mathbb KK. For a function H:E→KH:E\to\mathbb KH:E→K, call x∈Ex\in Ex∈E a critical zero of HHH if H(x)=0H(x)=0H(x)=0 and HHH is Fréchet differentiable at xxx with derivative 000.

Let T:E→ET:E\to ET:E→E be a K\mathbb KK-linear bijection which is continuous with continuous inverse, let F,G:E→KF,G:E\to\mathbb KF,G:E→K be arbitrary functions, and let k∈Kk\in\mathbb Kk∈K, k≠0k\ne0k=0, satisfy G(Tx)=k F(x)G(Tx)=k\,F(x)G(Tx)=kF(x) for all x∈Ex\in Ex∈E. Then for every x∈Ex\in Ex∈E

Tx is a critical zero of G  ⟺  x is a critical zero of F.Tx\ \text{is a critical zero of}\ G\iff x\ \text{is a critical zero of}\ F.Tx is a critical zero of G⟺x is a critical zero of F.

This is the invariance principle for the homogeneous Jacobian condition that defines the singular points of the curve Vα⊂P1×P1V_\alpha\subset\mathbb P^1\times\mathbb P^1Vα​⊂P1×P1 of Lemma 4. The formalization applies it to the linear maps induced by Möbius matrices, to rescalings of homogeneous coordinates, to changes of chart and to the exchange of the two factors of P1×P1\mathbb P^1\times\mathbb P^1P1×P1. No regularity of FFF or GGG is assumed.

Formalization Note: the condition is H x = 0 ∧ HasFDerivAt H 0 x. Using HasFDerivAt rather than the totalized derivative fderiv means that a point where HHH is not differentiable is never a critical zero. TTT is a continuous linear equivalence E ≃L[𝕜] E.

Preamble
import Definitions.Def_CurveSymmetry_01_RealLoci
import Definitions.Def_CurveSymmetry_02_FamilyBasics
import Definitions.Def_CurveSymmetry_03_IsometriesAndCharts
import Mathlib.Algebra.MvPolynomial.Nilpotent
import Mathlib.Algebra.MvPolynomial.NoZeroDivisors
import Mathlib.Algebra.MvPolynomial.PDeriv
import Mathlib.Algebra.Polynomial.FieldDivision
import Mathlib.Algebra.Polynomial.Reverse
import Mathlib.Analysis.Calculus.FDeriv.Equiv
import Mathlib.Analysis.Calculus.FDeriv.Mul
import Mathlib.Analysis.Complex.Isometry
import Mathlib.Analysis.Complex.OperatorNorm
import Mathlib.Analysis.Complex.Polynomial.Basic
import Mathlib.Analysis.Normed.Affine.MazurUlam
import Mathlib.Data.Complex.Basic
import Mathlib.FieldTheory.Separable
import Mathlib.RingTheory.MvPolynomial.Homogeneous
import Mathlib.RingTheory.MvPolynomial.IrreducibleQuadratic
import Mathlib.RingTheory.Polynomial.Eisenstein.Criterion
import Mathlib.RingTheory.Polynomial.GaussLemma
import Mathlib.RingTheory.RootsOfUnity.Complex
import Mathlib.RingTheory.RootsOfUnity.PrimitiveRoots
import Mathlib.Tactic
import Mathlib.Topology.Algebra.Module.FiniteDimension
import Mathlib.Topology.Compactification.OnePoint.ProjectiveLine

open CurveSymmetry
set_option autoImplicit false
Formal statement
theorem CurveSymmetry.criticalZero_transport {𝕜 E : Type*} [NontriviallyNormedField 𝕜]
    [NormedAddCommGroup E] [NormedSpace 𝕜 E]
    (T : E ≃L[𝕜] E) {F G : E → 𝕜} {k : 𝕜} (hk : k ≠ 0)
    (he : ∀ x, G (T x) = k * F x) (x : E) :
    CriticalZero G (T x) ↔ CriticalZero F x := by sorry
Source
C. Perassi, Sharp symmetry bounds for real algebraic curves (note): lemma of the formalization, used for Theorem 1 (p. 1), Theorem 2 (p. 2), Lemma 4 (p. 3), https://github.com/carlok/curve-symmetry-lean/blob/d99bc17a1c397956c05d7417de50f9beed56580f/sharp_symmetry_bounds.pdf. Lean: https://github.com/carlok/curve-symmetry-lean/blob/d99bc17a1c397956c05d7417de50f9beed56580f/lean/HomogeneousDifferential.lean (C. Perassi)

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