Body-Pin Rigidity

8.3. The orbit dimension drop🔗

Lemma8.3.1
Group: The paper's assembly argument: the partition, the selection lemma, the orbit drop, the properness of the exceptional locus, and the final assembly. (4)
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Definition 8.1.1
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Lemma 8.4.1
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✓L∃∀N

Suppose \mathbb{G}_m acts freely on a quasi-affine variety X of finite type and a morphism \pi : X \to Y is constant on each orbit. Then \dim \pi(X) \le \dim X - 1. (Zheng, 2026, Lemma 6.4)

Lean code for Lemma8.3.1●2 theorems
  • theorem RB31E2E.NullCellulePolynomial.homogeneousPrime_height_lt_of_irrelevant_mem_not_mem.{u_1}
      {k : Type u_1} [Field k] {n : ℕ} (P : Ideal (MvPolynomial (Fin n) k))
      [P.IsPrime]
      (hPhom :
        Ideal.IsHomogeneous (MvPolynomial.homogeneousSubmodule (Fin n) k) P)
      (s : MvPolynomial (Fin n) k)
      (hsIrrelevant :
        s ∈ RB31E2E.NullCellulePolynomial.finiteIrrelevantIdeal n)
      (hsP : s ∉ P) : P.height < ↑n
    theorem RB31E2E.NullCellulePolynomial.homogeneousPrime_height_lt_of_irrelevant_mem_not_mem.{u_1}
      {k : Type u_1} [Field k] {n : ℕ}
      (P : Ideal (MvPolynomial (Fin n) k))
      [P.IsPrime]
      (hPhom :
        Ideal.IsHomogeneous
          (MvPolynomial.homogeneousSubmodule
            (Fin n) k)
          P)
      (s : MvPolynomial (Fin n) k)
      (hsIrrelevant :
        s ∈
          RB31E2E.NullCellulePolynomial.finiteIrrelevantIdeal
            n)
      (hsP : s ∉ P) : P.height < ↑n
    A homogeneous prime avoiding any specified member of the irrelevant
    ideal has height strictly below the number of ambient variables. 
  • theorem RB31E2E.NullCellulePolynomial.finiteIrrelevantIdeal_height.{u_1}
      {k : Type u_1} [Field k] (n : ℕ) :
      (RB31E2E.NullCellulePolynomial.finiteIrrelevantIdeal n).height = ↑n
    theorem RB31E2E.NullCellulePolynomial.finiteIrrelevantIdeal_height.{u_1}
      {k : Type u_1} [Field k] (n : ℕ) :
      (RB31E2E.NullCellulePolynomial.finiteIrrelevantIdeal
            n).height =
        ↑n
    The height of the irrelevant ideal in `n` variables is exactly `n`.
    
    The lower bound is the explicit chain obtained by adjoining the variables
    one at a time.  The upper bound uses that the ideal is generated by the `n`
    coordinate variables. 

The paper proves this from the fibre-dimension theorem: the group is connected, so it preserves each irreducible component, and every one-dimensional orbit lies in a fibre of \pi. The formalization proves no statement of this shape, and the register has the entry. The point-set content (the common-scaling action is free on every grounded nonzero assignment, units_commonScale_injective_of_ne_zero) is proved in a module whose own comment defers the conversion into a dimension inequality, and nothing reachable from the root theorem uses it. What stands in for the orbit drop is homogeneity. The compatibility equations are homogeneous in the twist variables, so the bad locus of a fixed partition is a homogeneous ideal in the twist coordinates over the pin coefficients, and a homogeneous prime avoiding any element of the irrelevant ideal — here a distinctness denominator, a product of twist-difference coordinates and so of positive degree — has height strictly below the number of twist variables, by homogeneousPrime_height_lt_of_irrelevant_mem_not_mem together with the computation of the irrelevant ideal's height in finiteIrrelevantIdeal_height. The strict inequality is the paper's -1.