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The gradient of η\etaη: ∇η(x,s)=((s+rg(x))∇g(x), g(x))\nabla\eta(x,s)=((s+rg(x))\nabla g(x),\ g(x))∇η(x,s)=((s+rg(x))∇g(x), g(x)) where s+rg(x)≥0s+rg(x)\ge 0s+rg(x)≥0 and (0,−s/r)(0,-s/r)(0,−s/r) where s+rg(x)≤0s+rg(x)\le 0s+rg(x)≤0

Proved
NonsmoothNewton.AugLagrangian.eta_fderiv_formula

by WillR · Sep 29, 2026 · Mathlib 0df444a (Lean v4.33.1)

augmented-lagrangiancalculusnonsmooth-analysissource-faithful-child

Let r>0r>0r>0 and g:Rn→Rg:\mathbb{R}^n\to\mathbb{R}g:Rn→R be C2C^2C2, and assume η\etaη is C1C^1C1. Then the gradient of η\etaη at (x,s)(x,s)(x,s) is ((s+rg(x))∇g(x), g(x))\bigl((s+rg(x))\nabla g(x),\,g(x)\bigr)((s+rg(x))∇g(x),g(x)) where s+rg(x)≥0s+rg(x)\ge 0s+rg(x)≥0, and (0, −sr)\bigl(0,\,-\frac sr\bigr)(0,−rs​) where s+rg(x)≤0s+rg(x)\le 0s+rg(x)≤0. On the open regions s+rg(x)>0s+rg(x)>0s+rg(x)>0 and s+rg(x)<0s+rg(x)<0s+rg(x)<0 the function η\etaη is the polynomial s g(x)+r2g(x)2s\,g(x)+\frac r2 g(x)^2sg(x)+2r​g(x)2 and respectively −12rs2-\frac1{2r}s^2−2r1​s2, whose differentials are the displayed expressions; continuity of ∇η\nabla\eta∇η supplied by C1C^1C1 extends the identity across the surface s+rg(x)=0s+rg(x)=0s+rg(x)=0, and there the two formulas coincide because g(x)=−s/rg(x)=-s/rg(x)=−s/r. This is the displayed gradient formula, item 2 of Theorem 4.1.

Formal statement
import Mathlib
import Definitions.Def_NonsmoothNewton_Shared_clarkeJac
import Definitions.Def_NonsmoothNewton_AugLagrangian_SemismoothAt
import Definitions.Def_NonsmoothNewton_AugLagrangian_augLagrangian

namespace NonsmoothNewton.AugLagrangian

/-- Child of `eta_C1_grad_locLip`, second step of Qi-Sun (1993), Section 4, proof of Theorem 4.1,
pp. 363-364: the displayed formula for $\nabla\eta$ (item 2 of the theorem).

The gradient is represented by the Fréchet derivative, a continuous linear functional on
$\mathbb{R}^n\times\mathbb{R}$: in the first case $(h,\alpha)\mapsto (s+rg(x))\,Dg(x)h+g(x)\,\alpha$,
and in the second $(h,\alpha)\mapsto -\frac sr\,\alpha$. The two agree where $s+rg(x)=0$, because
there $g(x)=-\frac sr$, so the two non-strict cases are consistent. -/
theorem eta_fderiv_formula {n : ℕ} (r : ℝ) (hr : 0 < r)
    (g : EuclideanSpace ℝ (Fin n) → ℝ) (hg : ContDiff ℝ 2 g)
    (hη : ContDiff ℝ 1 (eta r g)) :
    (∀ z : EuclideanSpace ℝ (Fin n) × ℝ, 0 ≤ z.2 + r * g z.1 →
      fderiv ℝ (eta r g) z =
        (z.2 + r * g z.1) • (fderiv ℝ g z.1).comp
            (ContinuousLinearMap.fst ℝ (EuclideanSpace ℝ (Fin n)) ℝ)
          + g z.1 • ContinuousLinearMap.snd ℝ (EuclideanSpace ℝ (Fin n)) ℝ) ∧
    (∀ z : EuclideanSpace ℝ (Fin n) × ℝ, z.2 + r * g z.1 ≤ 0 →
      fderiv ℝ (eta r g) z =
        (-(z.2 / r)) • ContinuousLinearMap.snd ℝ (EuclideanSpace ℝ (Fin n)) ℝ) := by sorry

end NonsmoothNewton.AugLagrangian
Source
Qi, Sun, A nonsmooth version of Newton's method, Math. Programming 58 (1993), pp. 363-364, Section 4, proof of Theorem 4.1, the display of ∇η\nabla\eta∇η (item 2 of the theorem).

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